master
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a Code for the Combination of Indirect and Direct Constraints on High Energy Physics Models |
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master
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a Code for the Combination of Indirect and Direct Constraints on High Energy Physics Models |
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A model class for new physics in the form of the dimension-six effective Lagrangian. More...
#include <NPSMEFTd6.h>
Inheritance diagram for NPSMEFTd6:A model class for new physics in the form of the dimension-six effective Lagrangian.
This is a Model class containing parameters and functions associated with the general dimension-six effective Lagrangian. (Use the model name "NPSMEFTd6_LFU_QFU" to assume lepton and quark flavour universality)
In this class we consider the dimension-six effective Lagrangian
\[ \mathcal{L}_\mathrm{eff} = \mathcal{L}_\mathrm{SM} + \sum_i \frac{C_i}{\Lambda^2} \mathcal{O}_i. \]
The implementation is written in the basis of [Grzadkowski:2010es]. For convenience, the parameterization also includes operators appearing in other common bases. In particular, the complete set of parameters contains 4 redundancies, given by the coefficients \(C_{2B,2W,DHB,DHW,DB,DW} \), which correspond to operators not included in the basis of [Grzadkowski:2010es]. For meaningful physical results one must make sure to include only a complete set of interactions in a given analysis.
After creating an instance of the current class with the constructor NPSMEFTd6(), it is required to call the initialization method InitializeModel(). In the Monte Carlo run, the constructor as well as the initialization method are called in InputParser::ReadParameters().
The model parameters of NPSMEFTd6 are summarized below:
| Label | LaTeX symbol | Description |
|---|---|---|
| CG | \(C_{G} \) | The coefficient of the operator \({\cal O}_{G}=f_{ABC}G_{\mu}^{A\nu} G_{\nu}^{B\rho}W_{\rho}^{C\mu}\). |
| CW | \(C_{W} \) | The coefficient of the operator \({\cal O}_{W}=\varepsilon_{abc}W_{\mu}^{a\nu} W_{\nu}^{b\rho}W_{\rho}^{b\mu}\). |
| C2B | \(C_{2B} \) | The coefficient of the operator \({\cal O}_{2B}=\frac 12 (\partial_\rho B_{\mu\nu})^2\). (Implemented via EOM.) |
| C2W | \(C_{2W} \) | The coefficient of the operator \({\cal O}_{2W}=\frac 12 (D_\rho W_{\mu\nu}^{a})^2\). (Implemented via EOM.) |
| C2BS | \(C_{2B}^{SILH} \) | The coefficient of the SILH operator \({\cal O}_{2B}^{SILH}=\frac 12 (\partial^\mu B_{\mu\nu})(\partial_\rho B^{\rho\nu})\). (Implemented via EOM.) |
| C2WS | \(C_{2W}^{SILH} \) | The coefficient of the operator \({\cal O}_{2W}^{SILH}=\frac 12 (D_\mu W^{a~\!\mu\nu})(D^\rho W_{\rho\nu}^{a})\). (Implemented via EOM.) |
| CHG | \(C_{HG} \) | The coefficient of the operator \({\cal O}_{HG}=\big(H^\dagger H\big)G_{\mu\nu}^A G^{A\mu\nu}\). |
| CHW | \(C_{HW} \) | The coefficient of the operator \({\cal O}_{HW}=\big(H^\dagger H\big)W_{\mu\nu}^a W^{a\mu\nu}\). |
| CHB | \(C_{HB} \) | The coefficient of the operator \({\cal O}_{HB}=\big(H^\dagger H\big)B_{\mu\nu} B^{\mu\nu}\). |
| CDHB | \(C_{DHB} \) | The coefficient of the operator \({\cal O}_{DHB}=i\big(D^\mu H^\dagger D^\nu H\big) B_{\mu\nu}\). |
| CDHW | \(C_{DHW}\) | The coefficient of the operator \({\cal O}_{DHW}=i\big(D^\mu H^\dagger \sigma^a D^\nu H\big) W_{\mu\nu}^a\). |
| CDB | \(C_{DB} \) | The coefficient of the operator \({\cal O}_{DB}=\frac{i}{2}\big(H^\dagger \overset{\leftrightarrow}{D}^\mu H\big) \partial^\nu B_{\mu\nu}\). (Implemented via EOM.) |
| CDW | \(C_{DW}\) | The coefficient of the operator \({\cal O}_{DW}=\frac{i}{2}\big(H^\dagger \overset{\leftrightarrow}{D}^{a~\!\mu} H\big) D^\nu W_{\mu\nu}^a\). (Implemented via EOM.) |
| CWB | \(C_{WB} \) | The coefficient of the operator \({\cal O}_{HWB}=\big(H^\dagger\sigma^a H\big)W_{\mu\nu}^a B^{\mu\nu}\). |
| CHD | \(C_{HD}\) | The coefficient of the operator \({\cal O}_{HD}=\big|H^\dagger D_\mu H\big|^2\). |
| CT | \(C_{T}\) | The coefficient of the operator \({\cal O}_{T}=\frac{1}{2} \big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big)^2\). |
| CHbox | \(C_{H\Box}\) | The coefficient of the operator \({\cal O}_{H\Box}=\big(H^\dagger H\big)\Box\big(H^\dagger H\big)\). |
| CH | \(C_{H}\) | The coefficient of the operator \({\cal O}_{H}=\big(H^\dagger H\big)^3\). |
| CHL1_kk, CHL1_klr, CHL1_kli | \( (C_{HL}^{(1)})_{kk}, \mbox{Re}\big[(C_{HL}^{(1)})_{kl}\big], \mbox{Im}\big[(C_{HL}^{(1)})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HL}^{(1)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{L^i}\,\gamma^\mu L^j\big)\), for \(i,j=1,2,3\). |
| CHL3_kk, CHL3_klr, CHL3_kli | \( (C_{HL}^{(3)})_{kk}, \mbox{Re}\big[(C_{HL}^{(3)})_{kl}\big], \mbox{Im}\big[(C_{HL}^{(3)})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HL}^{(3)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{L^i}\,\gamma^\mu \sigma^a L^j\big)\), for \(i,j=1,2,3\). |
| CHe_kk, CHe_klr, CHe_kli | \( (C_{He})_{kk}, \mbox{Re}\big[(C_{He})_{kl}\big], \mbox{Im}\big[(C_{He})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{He})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{E^i}\,\gamma^\mu E^j\big)\), for \(i,j=1,2,3\). |
| CHQ1_kk, CHQ1_klr, CHQ1_kli | \( (C_{HQ}^{(1)})_{kk}, \mbox{Re}\big[(C_{HQ}^{(1)})_{kl}\big], \mbox{Im}\big[(C_{HQ}^{(1)})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HQ}^{(1)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{Q^i}\,\gamma^\mu Q^j\big)\), for \(i,j=1,2,3\). |
| CHQ3_kk, CHQ3_klr, CHQ3_kli | \( (C_{HQ}^{(3)})_{kk}, \mbox{Re}\big[(C_{HQ}^{(3)})_{kl}\big], \mbox{Im}\big[(C_{HQ}^{(3)})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HQ}^{(3)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{Q^i}\,\gamma^\mu \sigma^a Q^j\big)\), for \(i,j=1,2,3\). |
| CHu_kk, CHu_klr, CHu_kli | \( (C_{Hu})_{kk}, \mbox{Re}\big[(C_{Hu})_{kl}\big], \mbox{Im}\big[(C_{Hu})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hu})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{U^i}\,\gamma^\mu U^j\big)\), for \(i,j=1,2,3\). |
| CHd_kk, CHd_klr, CHd_kli | \( (C_{Hd})_{kk}, \mbox{Re}\big[(C_{Hd})_{kl}\big], \mbox{Im}\big[(C_{Hd})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hd})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{D^i}\,\gamma^\mu D^j\big)\), for \(i,j=1,2,3\). |
| CHud_klr, CHud_kli | \(\mbox{Re}\big[(C_{Hud})_{kl}\big], \mbox{Im}\big[(C_{Hud})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hud})_{ij} =i\big(\widetilde{H}^\dagger D_\mu H\big) \big(\overline{U^i}\,\gamma^\mu D^j\big)\), for \(i,j=1,2,3\). |
| CeH_klr, CeH_kli | \(\mbox{Re}\big[(C_{eH})_{kl}\big], \mbox{Im}\big[(C_{eH})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eH})_{ij} =\big(H^\dagger H\big) \big(\overline{L^i}\,H E^j\big)\), for \(i,j=1,2,3\). |
| CuH_klr, CuH_kli | \(\mbox{Re}\big[(C_{uH})_{kl}\big], \mbox{Im}\big[(C_{uH})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uH})_{ij} =\big(H^\dagger H\big) \big(\overline{Q^i}\,\widetilde{H} U^j\big)\), for \(i,j=1,2,3\). |
| CdH_klr, CdH_kli | \(\mbox{Re}\big[(C_{dH})_{kl}\big], \mbox{Im}\big[(C_{dH})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dH})_{ij} =\big(H^\dagger H\big) \big(\overline{Q^i}\,H D^j\big)\), for \(i,j=1,2,3\). |
| CuG_klr, CuG_kli | \(\mbox{Re}\big[(C_{uG})_{kl}\big], \mbox{Im}\big[(C_{uG})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uG})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} T_A U^j\big)\widetilde{H} G_{\mu\nu}^A\), for \(i,j=1,2,3\). |
| CuW_klr, CuW_kli | \(\mbox{Re}\big[(C_{uW})_{kl}\big], \mbox{Im}\big[(C_{uW})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uW})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} \sigma_a U^j\big)\widetilde{H} W_{\mu\nu}^a\), for \(i,j=1,2,3\). |
| CuB_klr, CuB_kli | \(\mbox{Re}\big[(C_{uB})_{kl}\big], \mbox{Im}\big[(C_{uB})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uB})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} U^j\big)\widetilde{H} B_{\mu\nu}\), for \(i,j=1,2,3\). |
| CdG_klr, CdG_kli | \(\mbox{Re}\big[(C_{dG})_{kl}\big], \mbox{Im}\big[(C_{dG})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dG})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} T_A D^j\big)H G_{\mu\nu}^A\), for \(i,j=1,2,3\). |
| CdW_klr, CdW_kli | \(\mbox{Re}\big[(C_{dW})_{kl}\big], \mbox{Im}\big[(C_{dW})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dW})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} \sigma_a D^j\big)H W_{\mu\nu}^a\), for \(i,j=1,2,3\). |
| CdB_klr, CdB_kli | \(\mbox{Re}\big[(C_{dB})_{kl}\big], \mbox{Im}\big[(C_{dB})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dB})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} D^j\big)H B_{\mu\nu}\), for \(i,j=1,2,3\). |
| CeW_klr, CeW_kli | \(\mbox{Re}\big[(C_{eW})_{kl}\big], \mbox{Im}\big[(C_{eW})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eW})_{ij} =\big(\overline{L^i}\sigma^{\mu\nu} \sigma_a E^j\big)H W_{\mu\nu}^a\), for \(i,j=1,2,3\). |
| CeB_klr, CeB_kli | \(\mbox{Re}\big[(C_{eB})_{kl}\big], \mbox{Im}\big[(C_{eB})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eB})_{ij} =\big(\overline{L^i}\sigma^{\mu\nu} E^j\big)H B_{\mu\nu}\), for \(i,j=1,2,3\). |
| CLL_1221, CLL_2112 | \((C_{LL})_{1221,2112}\) | The coefficient of the operator \(({\cal O}_{LL})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{L^k}\,\gamma_\mu L^l\big)\), for \(ijkl=1221,2112\). |
| CLQ1 | \(C_{LQ}^{(1)}\) | The coefficient of the operator \(({\cal O}_{LQ}^{(1)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{Q^k}\,\gamma_\mu Q^l\big)\). |
| CLQ3 | \(C_{LQ}^{(3)}\) | The coefficient of the operator \(({\cal O}_{LQ}^{(3)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu \sigma_a L^j\big) \big(\overline{Q^k}\,\gamma_\mu \sigma_a Q^l\big)\). |
| Cee | \(C_{EE}\) | The coefficient of the operator \(({\cal O}_{EE})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| Ceu | \(C_{EU}\) | The coefficient of the operator \(({\cal O}_{EU})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\). |
| Ced | \(C_{ED}\) | The coefficient of the operator \(({\cal O}_{ED})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\). |
| CLe | \(C_{LE}\) | The coefficient of the operator \(({\cal O}_{LE})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| CLu | \(C_{LU}\) | The coefficient of the operator \(({\cal O}_{LU})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\). |
| CLd | \(C_{LD}\) | The coefficient of the operator \(({\cal O}_{LD})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\). |
| CQe | \(C_{QE}\) | The coefficient of the operator \(({\cal O}_{QE})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| CQQ1_1133, CQQ1_1331, CQQ1_2233, CQQ1_2332, CQQ1_3333 | \(C_{QQ}^{(1)}\) | The coefficient of the operator \(({\cal O}_{QQ}^{(1)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{Q^k}\,\gamma_\mu Q^l\big)\). |
| CQQ3_1133, CQQ3_1331, CQQ3_2233, CQQ3_2332, CQQ3_3333 | \(C_{QQ}^{(3)}\) | The coefficient of the operator \(({\cal O}_{QQ}^{(3)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu \sigma_a Q^j\big) \big(\overline{Q^k}\,\gamma_\mu \sigma_a Q^l\big)\). |
| Cuu_1133, Cuu_1331, Cuu_2233, Cuu_2332, Cuu_3333 | \(C_{uu}\) | The coefficient of the operator \(({\cal O}_{uu})_{ijkl}=\big(\overline{u^i}\,\gamma^\mu u^j\big) \big(\overline{u^k}\,\gamma_\mu u^l\big)\). |
| Cud1_3311, Cud1_3322, Cud1_3333 | \(C_{ud}^{(1)}\) | The coefficient of the operator \(({\cal O}_{ud}^{(1)})_{ijkl}=\big(\overline{u^i}\,\gamma^\mu u^j\big) \big(\overline{d^k}\,\gamma_\mu d^l\big)\). |
| Cud8_3311, Cud8_3322, Cud8_3333 | \(C_{ud}^{(8)}\) | The coefficient of the operator \(({\cal O}_{ud}^{(8)})_{ijkl}=\big(\overline{u^i}\,\gamma^\mu T^A u^j\big) \big(\overline{d^k}\,\gamma_\mu T^A d^l\big)\). |
| CQu1_1133, CQu1_3311, CQu1_2233, CQu1_3322, CQu1_3333 | \(C_{Qu}^{(1)}\) | The coefficient of the operator \(({\cal O}_{Qu}^{(1)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{u^k}\,\gamma_\mu u^l\big)\). |
| CQu8_1133, CQu8_3311, CQu8_2233, CQu8_3322, CQu8_3333 | \(C_{Qu}^{(8)}\) | The coefficient of the operator \(({\cal O}_{Qu}^{(8)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu T^A Q^j\big) \big(\overline{u^k}\,\gamma_\mu T^A u^l\big)\). |
| CQd1_3311, CQd1_3322, CQd1_3333 | \(C_{Qd}^{(1)}\) | The coefficient of the operator \(({\cal O}_{Qd}^{(1)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{d^k}\,\gamma_\mu d^l\big)\). |
| CQd8_3311, CQd8_3322, CQd8_3333 | \(C_{Qd}^{(8)}\) | The coefficient of the operator \(({\cal O}_{Qd}^{(8)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu T^A Q^j\big) \big(\overline{d^k}\,\gamma_\mu T^A d^l\big)\). |
| CQuQd1_3333 | \(C_{QuQd}^{(1)}\) | The coefficient of the operator \(({\cal O}_{QuQd}^{(1)})_{ijkl}=\big(\overline{Q^i}\, u^j\big) i\sigma_2 \big(\overline{Q^k}^T\, d^l\big)\). |
| CQuQd8_3333 | \(C_{QuQd}^{(8)}\) | The coefficient of the operator \(({\cal O}_{QuQd}^{(8)})_{ijkl}=\big(\overline{Q^i}\, T^A u^j\big) i\sigma_2 \big(\overline{Q^k}^T\, T^A d^l\big)\). |
| Lambda_NP | \(\Lambda \) | The new physics scale. |
| BrHinv | Br \((H\to invisible)\) | The branching ratio of invisible Higgs decays. Only the absolute value of this parameter is considered.(Not part of the EFT. Only for tests.) |
| BrHexo | Br \((H\to exotic)\) | The branching ratio of exotic Higgs decays. Only the absolute value of this parameter is considered. (Not part of the EFT. Only for tests.) |
| dg1Z | \(\delta g_{1Z}\) | Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.) |
| dKappaga | \(\delta \kappa_{\gamma}\) | Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.) |
| lambZ | \(\lambda_{Z}\) | Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.) |
| eXint | \(\varepsilon_{X}^{int}\) | The relative intrinsic theoretical uncertainty for the process X. (Only for Higgs observables and assumed to be constant in the energy.) |
| eXpar | \(\varepsilon_{X}^{par}\) | The relative parametric theoretical uncertainty for the process X. (Only for Higgs observables and assumed to be constant in the energy.) |
| eVBFE_i | \(\varepsilon_{VBF}^i(E)\) | The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the VBF production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i=g_{HZZ}^{(1,2,3)}, g_{HZA}^{(1,2)}, g_{HAA}, g_{HWW}^{(1,2,3)}, g_{Hgg}, g_{HZuu,HZdd}^{L,R}, g_{HWud}^{L}, g_{Zuu,Zdd}^{L,R}, g_{Wud}^{L})\) |
| eWHE_i | \(\varepsilon_{WH}^i(E)\) | The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the WH production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i= g_{HWW}^{(1,2,3)}, g_{HWud}^{L}, g_{Wud}^{L})\) |
| eZHE_i | \(\varepsilon_{ZH}^i(E)\) | The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the ZH production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i=g_{HZZ}^{(1,2,3)}, g_{HZA}^{(1,2)}, g_{HZuu,HZdd}^{L,R}, g_{Zuu,Zdd}^{L,R})\) |
| ettHE_i | \(\varepsilon_{ttH}^i(E)\) | The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the ttH production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i= g_{Htt}, g_{Hgg})\) |
Where the hermitian derivatives are defined as
\[ H^\dagger i \overset{\leftrightarrow}{D}_\mu H\equiv H^\dagger i(D_\mu - \overset{\leftarrow}{D}_\mu)H \]
and
\[ H^\dagger i \overset{\leftrightarrow}{D^a_\mu} H\equiv H^\dagger i (\sigma^a D_\mu - \overset{\leftarrow}{D}_\mu \sigma^a)H. \]
Alternatively, when using the model name "NPSMEFTd6_LFU_QFU", where lepton and quark flavour universality are assumed (except for \((C_{fH})_{ij},~f=e,u,d\) which are assumed to be diagonal only), the parameters to be used as inputs for the dimension six coefficients are the following:
| Label | LaTeX symbol | Description |
|---|---|---|
| CG | \(C_{G} \) | The coefficient of the operator \({\cal O}_{G}=f_{ABC}G_{\mu}^{A\nu} G_{\nu}^{B\rho}W_{\rho}^{C\mu}\). |
| CW | \(C_{W} \) | The coefficient of the operator \({\cal O}_{W}=\varepsilon_{abc}W_{\mu}^{a\nu} W_{\nu}^{b\rho}W_{\rho}^{b\mu}\). |
| C2B | \(C_{2B} \) | The coefficient of the operator \({\cal O}_{2B}=\frac 12 (\partial_\rho B_{\mu\nu})^2\). (Implemented via EOM.) |
| C2W | \(C_{2W} \) | The coefficient of the operator \({\cal O}_{2W}=\frac 12 (D_\rho W_{\mu\nu}^{a})^2\). (Implemented via EOM.) |
| C2BS | \(C_{2B}^{SILH} \) | The coefficient of the SILH operator \({\cal O}_{2B}^{SILH}=\frac 12 (\partial^\mu B_{\mu\nu})(\partial_\rho B^{\rho\nu})\). (Implemented via EOM.) |
| C2WS | \(C_{2W}^{SILH} \) | The coefficient of the operator \({\cal O}_{2W}^{SILH}=\frac 12 (D_\mu W^{a~\!\mu\nu})(D^\rho W_{\rho\nu}^{a})\). (Implemented via EOM.) |
| CHG | \(C_{HG} \) | The coefficient of the operator \({\cal O}_{HG}=\big(H^\dagger H\big)G_{\mu\nu}^A G^{A\mu\nu}\). |
| CHW | \(C_{HW} \) | The coefficient of the operator \({\cal O}_{HW}=\big(H^\dagger H\big)W_{\mu\nu}^a W^{a\mu\nu}\). |
| CHB | \(C_{HB} \) | The coefficient of the operator \({\cal O}_{HB}=\big(H^\dagger H\big)B_{\mu\nu} B^{\mu\nu}\). |
| CDHB | \(C_{DHB} \) | The coefficient of the operator \({\cal O}_{DHB}=i\big(D^\mu H^\dagger D^\nu H\big) B_{\mu\nu}\). |
| CDHW | \(C_{DHW}\) | The coefficient of the operator \({\cal O}_{DHW}=i\big(D^\mu H^\dagger \sigma^a D^\nu H\big) W_{\mu\nu}^a\). |
| CDB | \(C_{DB} \) | The coefficient of the operator \({\cal O}_{DB}=\frac{i}{2}\big(H^\dagger \overset{\leftrightarrow}{D}^\mu H\big) \partial^\nu B_{\mu\nu}\). (Implemented via EOM.) |
| CDW | \(C_{DW}\) | The coefficient of the operator \({\cal O}_{DW}=\frac{i}{2}\big(H^\dagger \overset{\leftrightarrow}{D}^{a~\!\mu} H\big) D^\nu W_{\mu\nu}^a\). (Implemented via EOM.) |
| CWB | \(C_{WB} \) | The coefficient of the operator \({\cal O}_{HWB}=\big(H^\dagger\sigma^a H\big)W_{\mu\nu}^a B^{\mu\nu}\). |
| CHD | \(C_{HD}\) | The coefficient of the operator \({\cal O}_{HD}=\big|H^\dagger D_\mu H\big|^2\). |
| CT | \(C_{T}\) | The coefficient of the operator \({\cal O}_{T}=\frac{1}{2} \big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big)^2\). |
| CHbox | \(C_{H\Box}\) | The coefficient of the operator \({\cal O}_{H\Box}=\big(H^\dagger H\big)\Box\big(H^\dagger H\big)\). |
| CH | \(C_{H}\) | The coefficient of the operator \({\cal O}_{H}=\big(H^\dagger H\big)^3\). |
| CHL1 | \( (C_{HL}^{(1)})_{ii} \) | The coefficient of the operator \(({\cal O}_{HL}^{(1)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{L^i}\,\gamma^\mu L^i\big)\) (flavor universal). |
| CHL3 | \( (C_{HL}^{(3)})_{ii} \) | The coefficient of the operator \(({\cal O}_{HL}^{(3)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{L^i}\,\gamma^\mu \sigma^a L^i\big)\) (flavor universal). |
| CHe | \( (C_{He})_{ii} \) | The coefficient of the operator \(({\cal O}_{He})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{E^i}\,\gamma^\mu E^i\big)\) (flavor universal). |
| CHQ1 | \( (C_{HQ}^{(1)})_{ii} \) | The coefficient of the operator \(({\cal O}_{HQ}^{(1)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{Q^i}\,\gamma^\mu Q^i\big)\) (flavor universal). |
| CHQ3 | \( (C_{HQ}^{(3)})_{ii}\) | The coefficient of the operator \(({\cal O}_{HQ}^{(3)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{Q^i}\,\gamma^\mu \sigma^a Q^i\big)\) (flavor universal). |
| CHu | \( (C_{Hu})_{ii} \) | The coefficient of the operator \(({\cal O}_{Hu})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{U^i}\,\gamma^\mu U^i\big)\) (flavor universal). |
| CHd | \( (C_{Hd})_{ii} \) | The coefficient of the operator \(({\cal O}_{Hd})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{D^i}\,\gamma^\mu D^i\big)\) (flavor universal). |
| CHud_r, CHud_i | \(\mbox{Re}\big[(C_{Hud})_{ii}\big], \mbox{Im}\big[(C_{Hud})_{ii}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hud})_{ii} =i\big(\widetilde{H}^\dagger D_\mu H\big) \big(\overline{U^i}\,\gamma^\mu D^i\big)\) (flavor universal). |
| CeH_jjr, CeH_jji | \(\mbox{Re}\big[(C_{eH})_{jj}\big], \mbox{Im}\big[(C_{eH})_{jj}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eH})_{jj} =\big(H^\dagger H\big) \big(\overline{L^j}\,H E^j\big)\) (flavor universal). |
| CuH_jjr, CuH_jji | \(\mbox{Re}\big[(C_{uH})_{jj}\big], \mbox{Im}\big[(C_{uH})_{jj}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uH})_{jj} =\big(H^\dagger H\big) \big(\overline{Q^j}\,\widetilde{H} U^j\big)\) (flavor universal). |
| CdH_jjr, CdH_jji | \(\mbox{Re}\big[(C_{dH})_{jj}\big], \mbox{Im}\big[(C_{dH})_{jj}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dH})_{jj} =\big(H^\dagger H\big) \big(\overline{Q^j}\,H D^j\big)\) (flavor universal). |
| CuG_jjr, CuG_jji | \(\mbox{Re}\big[(C_{uG})_{jj}\big], \mbox{Im}\big[(C_{uG})_{jj}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uG})_{jj} =\big(\overline{Q^j}\sigma^{\mu\nu} T_A U^j\big)\widetilde{H} G_{\mu\nu}^A\) (flavor universal). |
| CuW_jjr, CuW_jji | \(\mbox{Re}\big[(C_{uW})_{jj}\big], \mbox{Im}\big[(C_{uW})_{jj}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uW})_{jj} =\big(\overline{Q^j}\sigma^{\mu\nu} \sigma_a U^j\big)\widetilde{H} W_{\mu\nu}^a\) (flavor universal). |
| CuB_jjr, CuB_jji | \(\mbox{Re}\big[(C_{uB})_{jj}\big], \mbox{Im}\big[(C_{uB})_{jj}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uB})_{jj} =\big(\overline{Q^j}\sigma^{\mu\nu} U^j\big)\widetilde{H} B_{\mu\nu}\) (flavor universal). |
| CdG_jjr, CdG_jji | \(\mbox{Re}\big[(C_{dG})_{jj}\big], \mbox{Im}\big[(C_{dG})_{jj}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dG})_{jj} =\big(\overline{Q^j}\sigma^{\mu\nu} T_A D^j\big)H G_{\mu\nu}^A\) (flavor universal). |
| CdW_jjr, CdW_jji | \(\mbox{Re}\big[(C_{dW})_{jj}\big], \mbox{Im}\big[(C_{dW})_{jj}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dW})_{jj} =\big(\overline{Q^j}\sigma^{\mu\nu} \sigma_a D^j\big)H W_{\mu\nu}^a\) (flavor universal). |
| CdB_jjr, CdB_jji | \(\mbox{Re}\big[(C_{dB})_{jj}\big], \mbox{Im}\big[(C_{dB})_{jj}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dB})_{jj} =\big(\overline{Q^j}\sigma^{\mu\nu} D^j\big)H B_{\mu\nu}\) (flavor universal). |
| CeW_jjr, CeW_jji | \(\mbox{Re}\big[(C_{eW})_{jj}\big], \mbox{Im}\big[(C_{eW})_{jj}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eW})_{jj} =\big(\overline{L^j}\sigma^{\mu\nu} \sigma_a E^j\big)H W_{\mu\nu}^a\) (flavor universal). |
| CeB_jjr, CeB_jji | \(\mbox{Re}\big[(C_{eB})_{jj}\big], \mbox{Im}\big[(C_{eB})_{jj}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eB})_{jj} =\big(\overline{L^j}\sigma^{\mu\nu} E^j\big)H B_{\mu\nu}\) (flavor universal). |
| CLL | \((C_{LL})_{1221,2112}\) | The coefficient of the operator \(({\cal O}_{LL})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{L^k}\,\gamma_\mu L^l\big)\), for \(ijkl=1221,2112\). |
| CLQ1 | \(C_{LQ}^{(1)}\) | The coefficient of the operator \(({\cal O}_{LQ}^{(1)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{Q^k}\,\gamma_\mu Q^l\big)\). |
| CLQ3 | \(C_{LQ}^{(3)}\) | The coefficient of the operator \(({\cal O}_{LQ}^{(3)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu \sigma_a L^j\big) \big(\overline{Q^k}\,\gamma_\mu \sigma_a Q^l\big)\). |
| Cee | \(C_{EE}\) | The coefficient of the operator \(({\cal O}_{EE})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| Ceu | \(C_{EU}\) | The coefficient of the operator \(({\cal O}_{EU})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\). |
| Ced | \(C_{ED}\) | The coefficient of the operator \(({\cal O}_{ED})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\). |
| CLe | \(C_{LE}\) | The coefficient of the operator \(({\cal O}_{LE})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| CLu | \(C_{LU}\) | The coefficient of the operator \(({\cal O}_{LU})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\). |
| CLd | \(C_{LD}\) | The coefficient of the operator \(({\cal O}_{LD})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\). |
| CQe | \(C_{QE}\) | The coefficient of the operator \(({\cal O}_{QE})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| CQQ1 | \(C_{QQ}^{(1)}\) | The coefficient of the operator \(({\cal O}_{QQ}^{(1)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{Q^k}\,\gamma_\mu Q^l\big)\). |
| CQQ3 | \(C_{QQ}^{(3)}\) | The coefficient of the operator \(({\cal O}_{QQ}^{(3)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu \sigma_a Q^j\big) \big(\overline{Q^k}\,\gamma_\mu \sigma_a Q^l\big)\). |
| Cuu | \(C_{uu}\) | The coefficient of the operator \(({\cal O}_{uu})_{ijkl}=\big(\overline{u^i}\,\gamma^\mu u^j\big) \big(\overline{u^k}\,\gamma_\mu u^l\big)\). |
| Cud1 | \(C_{ud}^{(1)}\) | The coefficient of the operator \(({\cal O}_{ud}^{(1)})_{ijkl}=\big(\overline{u^i}\,\gamma^\mu u^j\big) \big(\overline{d^k}\,\gamma_\mu d^l\big)\). |
| Cud8 | \(C_{ud}^{(8)}\) | The coefficient of the operator \(({\cal O}_{ud}^{(8)})_{ijkl}=\big(\overline{u^i}\,\gamma^\mu T^A u^j\big) \big(\overline{d^k}\,\gamma_\mu T^A d^l\big)\). |
| CQu1 | \(C_{Qu}^{(1)}\) | The coefficient of the operator \(({\cal O}_{Qu}^{(1)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{u^k}\,\gamma_\mu u^l\big)\). |
| CQu8 | \(C_{Qu}^{(8)}\) | The coefficient of the operator \(({\cal O}_{Qu}^{(8)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu T^A Q^j\big) \big(\overline{u^k}\,\gamma_\mu T^A u^l\big)\). |
| CQd1 | \(C_{Qd}^{(1)}\) | The coefficient of the operator \(({\cal O}_{Qd}^{(1)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{d^k}\,\gamma_\mu d^l\big)\). |
| CQd8 | \(C_{Qd}^{(8)}\) | The coefficient of the operator \(({\cal O}_{Qd}^{(8)})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu T^A Q^j\big) \big(\overline{d^k}\,\gamma_\mu T^A d^l\big)\). |
| CQuQd1 | \(C_{QuQd}^{(1)}\) | The coefficient of the operator \(({\cal O}_{QuQd}^{(1)})_{ijkl}=\big(\overline{Q^i}\, u^j\big) i\sigma_2 \big(\overline{Q^k}^T\, d^l\big)\). |
| CQuQd8 | \(C_{QuQd}^{(8)}\) | The coefficient of the operator \(({\cal O}_{QuQd}^{(8)})_{ijkl}=\big(\overline{Q^i}\, T^A u^j\big) i\sigma_2 \big(\overline{Q^k}^T\, T^A d^l\big)\). |
| Lambda_NP | \(\Lambda \) | The new physics scale. |
| BrHinv | Br \((H\to invisible)\) | The branching ratio of invisible Higgs decays. (Not part of the EFT. Only for tests.) |
| BrHexo | Br \((H\to exotic)\) | The branching ratio of exotic Higgs decays. (Not part of the EFT. Only for tests.) |
(The parameters associated to the theoretical uncertainties: \(\varepsilon_{X}^{int}\), \(\varepsilon_{X}^{par}\) and \(\varepsilon_{X}^i(E)\), are the same for both "NPSMEFTd6" and "NPSMEFTd6_LFU_QFU".)
The Flags of NPSMEFTd6 are summarized below:
| Label | Value | Description |
|---|---|---|
| QuadraticTerms | TRUE / FALSE | This flag is set to TRUE if the quadratic terms in Higgs cross sections and widths are switched on. The default value is FALSE; new physics contributions are linearized. |
| RotateCHWCHB | TRUE / FALSE | This flag is set to TRUE if using {sW2*CHW+cW2*CHB, -cW2*CHW+sW2*CHB} instead of {CHW, CHB} as floating parameters. The default value is FALSE. |
| PartialQFU | TRUE / FALSE | This flag is set to TRUE if using CHQ1_11=CHQ1_22, CHQ3_11=CHQ3_22, CHU_11=CHU_22, CHD_11=CHD_22, CHud_11=CHud_22.} Only applies in the Non QFU case. In that case only the (1,1) component is taken into account. The default value is FALSE. |
| FlavU3OfX | TRUE / FALSE | This flag is set to TRUE if using \(U(3)^5\) flavour symmetry relations in the coefficients of the operators \(O_{fH}\) and \(O_{fV}\). If TRUE, the operator coefficient is proportional to the corresponding Yukawa matrix (diagonal), with the proportionality coefficient given by the Model parameter corresponding to the coefficient of third family. (Implemented only for the real and diagonal elements of the \(O_{fH}\) and \(O_{fV}\) operators.) The default value is FALSE. |
| FlagUnivOfX | TRUE / FALSE | This flag is set to TRUE if using \(U(3)^5\) flavour symmetry relations in the coefficients of the operators \(O_{fH}\) and \(O_{fV}\) plus they are the same for all fermions. If TRUE, all the operator coefficients are proportional to the corresponding Yukawa matrix (diagonal), with the proportionality coefficient given by the Model parameter corresponding to the coefficients of third family for \(O_{uH}\) and \(O_{uV}\), respectively. (Implemented only for the real and diagonal elements of the \(O_{fH}\) and \(O_{fV}\) operators.) The default value is FALSE. |
| HiggsSM | TRUE / FALSE | This flag is set to TRUE if including dependence on small variations of the SM parameters (dependence is linearized). Available only in selected Higgs observables. The default value is FALSE. |
| LoopHd6 | TRUE / FALSE | This flag is set to TRUE if including modifications in the SM loops in Higgs observables due to the dim 6 interactions. The default value is FALSE. |
| LoopH3d6Quad | TRUE / FALSE | This flag is set to TRUE if including quadratic modifications in the SM loops in Higgs observables due to the dim 6 interactions that contribute to the trilinear Higgs coupling. Works independently of the flag QuadraticTerms (the quadratic contributions are also added if the latter is true). The default value is FALSE. |
| RGEciLLA | TRUE / FALSE | This flag is set to TRUE if including log-enhanced 1-loop corrections proportional to the dim-6 Wilson coefficients via renormalization group effects. Only valid working exactly inside the Warsaw basis. Logs evaluated at the top mass scale. (NOT ACTIVE YET. PLACEHOLDER.) The default value is FALSE. |
| MWinput | TRUE / FALSE | This auxiliary flag is used for setting the W mass as a SM input, instead of the electromagnetic constant parameter dAle5Mz. The default value is FALSE. This flag must be used together with the flag of the same name in StandardModel |
See the base classes of the current class.
Definition at line 1052 of file NPSMEFTd6.h.
Public Member Functions | |
| gslpp::complex | AH_f (double tau) const |
| Fermionic loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings. More... | |
| gslpp::complex | AH_W (double tau) const |
| W loop function entering in the calculation of the effective \(H\gamma\gamma\) coupling. More... | |
| gslpp::complex | AHZga_f (double tau, double lambda) const |
| Fermionic loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| gslpp::complex | AHZga_W (double tau, double lambda) const |
| W loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| virtual const double | alphaMz () const |
| The electromagnetic coupling at the \(Z\)-mass scale. More... | |
| virtual const double | aPskPol (double sqrt_s, double Pol_em, double Pol_ep) const |
| the angular parameter \(a\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]). More... | |
| virtual const double | AuxObs_NP1 () const |
| Auxiliary observable AuxObs_NP1 (See code for details.) More... | |
| virtual const double | AuxObs_NP10 () const |
| Auxiliary observable AuxObs_NP10 (See code for details.) More... | |
| virtual const double | AuxObs_NP11 () const |
| Auxiliary observable AuxObs_NP11 (See code for details.) More... | |
| virtual const double | AuxObs_NP12 () const |
| Auxiliary observable AuxObs_NP12 (See code for details.) More... | |
| virtual const double | AuxObs_NP13 () const |
| Auxiliary observable AuxObs_NP13. More... | |
| virtual const double | AuxObs_NP14 () const |
| Auxiliary observable AuxObs_NP14. More... | |
| virtual const double | AuxObs_NP15 () const |
| Auxiliary observable AuxObs_NP15. More... | |
| virtual const double | AuxObs_NP16 () const |
| Auxiliary observable AuxObs_NP16. More... | |
| virtual const double | AuxObs_NP17 () const |
| Auxiliary observable AuxObs_NP17. More... | |
| virtual const double | AuxObs_NP18 () const |
| Auxiliary observable AuxObs_NP18. More... | |
| virtual const double | AuxObs_NP19 () const |
| Auxiliary observable AuxObs_NP19. More... | |
| virtual const double | AuxObs_NP2 () const |
| Auxiliary observable AuxObs_NP2 (See code for details.) More... | |
| virtual const double | AuxObs_NP20 () const |
| Auxiliary observable AuxObs_NP20. More... | |
| virtual const double | AuxObs_NP21 () const |
| Auxiliary observable AuxObs_NP21 (See code for details.) More... | |
| virtual const double | AuxObs_NP22 () const |
| Auxiliary observable AuxObs_NP22 (See code for details.) More... | |
| virtual const double | AuxObs_NP23 () const |
| Auxiliary observable AuxObs_NP23. More... | |
| virtual const double | AuxObs_NP24 () const |
| Auxiliary observable AuxObs_NP24. More... | |
| virtual const double | AuxObs_NP25 () const |
| Auxiliary observable AuxObs_NP25. More... | |
| virtual const double | AuxObs_NP26 () const |
| Auxiliary observable AuxObs_NP26. More... | |
| virtual const double | AuxObs_NP27 () const |
| Auxiliary observable AuxObs_NP27. More... | |
| virtual const double | AuxObs_NP28 () const |
| Auxiliary observable AuxObs_NP28. More... | |
| virtual const double | AuxObs_NP29 () const |
| Auxiliary observable AuxObs_NP29. More... | |
| virtual const double | AuxObs_NP3 () const |
| Auxiliary observable AuxObs_NP3 (See code for details.) More... | |
| virtual const double | AuxObs_NP30 () const |
| Auxiliary observable AuxObs_NP30. More... | |
| virtual const double | AuxObs_NP4 () const |
| Auxiliary observable AuxObs_NP4 (See code for details.) More... | |
| virtual const double | AuxObs_NP5 () const |
| Auxiliary observable AuxObs_NP5 (See code for details.) More... | |
| virtual const double | AuxObs_NP6 () const |
| Auxiliary observable AuxObs_NP6 (See code for details.) More... | |
| virtual const double | AuxObs_NP7 () const |
| Auxiliary observable AuxObs_NP7 (See code for details.) More... | |
| virtual const double | AuxObs_NP8 () const |
| Auxiliary observable AuxObs_NP8 (See code for details.) More... | |
| virtual const double | AuxObs_NP9 () const |
| Auxiliary observable AuxObs_NP9 (See code for details.) More... | |
| virtual const double | bPskPol (double sqrt_s, double Pol_em, double Pol_ep) const |
| the angular parameter \(b\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]). More... | |
| virtual const double | Br_H_exo () const |
| The branching ratio of the of the Higgs into exotic particles. More... | |
| virtual const double | Br_H_inv () const |
| The branching ratio of the of the Higgs into invisible particles. More... | |
| virtual const double | Br_H_inv_NP () const |
| The branching ratio of the of the Higgs into invisible particles (only invisible new particles). More... | |
| virtual const double | BrH2d2dRatio () const |
| The ratio of the Br \((H\to 2d2d)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2e2muRatio () const |
| The ratio of the Br \((H\to 2e 2\mu)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2e2vRatio () const |
| The ratio of the Br \((H\to 2e2v)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2evRatio () const |
| The ratio of the Br \((H\to 2ev)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2L2dRatio () const |
| The ratio of the Br \((H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2L2LRatio () const |
| The ratio of the Br \((H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2L2uRatio () const |
| The ratio of the Br \((H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2L2v2Ratio () const |
| The ratio of the Br \((H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2L2vRatio () const |
| The ratio of the Br \((H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2l2vRatio () const |
| The ratio of the Br \((H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2Lv2Ratio () const |
| The ratio of the Br \((H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2LvRatio () const |
| The ratio of the Br \((H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2mu2vRatio () const |
| The ratio of the Br \((H\to 2\mu 2v)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2muvRatio () const |
| The ratio of the Br \((H\to 2ev)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2u2dRatio () const |
| The ratio of the Br \((H\to 2u2d)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2u2uRatio () const |
| The ratio of the Br \((H\to 2u2u)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2udRatio () const |
| The ratio of the Br \((H\to 2ud)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2v2dRatio () const |
| The ratio of the Br \((H\to 2v2d)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2v2uRatio () const |
| The ratio of the Br \((H\to 2v2u)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH2v2vRatio () const |
| The ratio of the Br \((H\to 2v2v)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH4dRatio () const |
| The ratio of the Br \((H\to 4d)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH4eRatio () const |
| The ratio of the Br \((H\to 4e)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH4fRatio () const |
| The ratio of the Br \((H\to 4f)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH4L2Ratio () const |
| The ratio of the Br \((H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrH4LRatio () const |
| The ratio of the Br \((H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrH4lRatio () const |
| The ratio of the Br \((H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrH4muRatio () const |
| The ratio of the Br \((H\to 4\mu)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH4uRatio () const |
| The ratio of the Br \((H\to 4u)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrH4vRatio () const |
| The ratio of the Br \((H\to 4v)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHbbRatio () const |
| The ratio of the Br \((H\to b\bar{b})\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHccRatio () const |
| The ratio of the Br \((H\to c\bar{c})\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHevmuvRatio () const |
| The ratio of the Br \((H\to e\nu \mu\nu)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHgagaRatio () const |
| The ratio of the Br \((H\to \gamma\gamma)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHggRatio () const |
| The ratio of the Br \((H\to gg)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHll_vvorjjRatio () const |
| The ratio of the Br \((H\to l l \nu\nu, l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrHlv_lvorjjRatio () const |
| The ratio of the Br \((H\to l \nu l \nu, l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrHlvjjRatio () const |
| The ratio of the Br \((H\to l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrHLvudRatio () const |
| The ratio of the Br \((H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrHLvvLRatio () const |
| The ratio of the Br \((H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrHmumuRatio () const |
| The ratio of the Br \((H\to \mu^+\mu^-)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHtautauRatio () const |
| The ratio of the Br \((H\to \tau^+\tau^-)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHtoinvRatio () const |
| The ratio of the Br \((H\to invisible)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHudduRatio () const |
| The ratio of the Br \((H\to uddu)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHvisRatio () const |
| The ratio of the Br \((H\to visible)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHVVRatio () const |
| The ratio of the Br \((H\to VV)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHWW4fRatio () const |
| The ratio of the Br \((H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| virtual const double | BrHWWRatio () const |
| The ratio of the Br \((H\to WW)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHZgaeeRatio () const |
| The ratio of the Br \((H\to Z\gamma\to ee\gamma)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHZgallRatio () const |
| The ratio of the Br \((H\to Z\gamma\to ll\gamma)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| virtual const double | BrHZgamumuRatio () const |
| The ratio of the Br \((H\to Z\gamma\to \mu\mu\gamma)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHZgaRatio () const |
| The ratio of the Br \((H\to Z\gamma)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrHZZ4fRatio () const |
| The ratio of the Br \((H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| virtual const double | BrHZZRatio () const |
| The ratio of the Br \((H\to ZZ)\) in the current model and in the Standard Model. More... | |
| virtual const double | BrW (const Particle fi, const Particle fj) const |
| The branching ratio of the \(W\) boson decaying into a SM fermion pair, \(Br(W\to f_i f_j)\). More... | |
| const double | CeeLL_bottom () const |
| const double | CeeLL_charm () const |
| const double | CeeLL_down () const |
| const double | CeeLL_e () const |
| const double | CeeLL_mu () const |
| const double | CeeLL_strange () const |
| const double | CeeLL_tau () const |
| const double | CeeLL_top () const |
| const double | CeeLL_up () const |
| const double | CeeLR_bottom () const |
| const double | CeeLR_charm () const |
| const double | CeeLR_down () const |
| const double | CeeLR_e () const |
| const double | CeeLR_mu () const |
| const double | CeeLR_strange () const |
| const double | CeeLR_tau () const |
| const double | CeeLR_top () const |
| const double | CeeLR_up () const |
| const double | CeeRL_bottom () const |
| const double | CeeRL_charm () const |
| const double | CeeRL_down () const |
| const double | CeeRL_e () const |
| const double | CeeRL_mu () const |
| const double | CeeRL_strange () const |
| const double | CeeRL_tau () const |
| const double | CeeRL_top () const |
| const double | CeeRL_up () const |
| const double | CeeRR_bottom () const |
| const double | CeeRR_charm () const |
| const double | CeeRR_down () const |
| const double | CeeRR_e () const |
| const double | CeeRR_mu () const |
| const double | CeeRR_strange () const |
| const double | CeeRR_tau () const |
| const double | CeeRR_top () const |
| const double | CeeRR_up () const |
| virtual const double | CEWHd11 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{11}\). More... | |
| virtual const double | CEWHd22 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{22}\). More... | |
| virtual const double | CEWHd33 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{33}\). More... | |
| virtual const double | CEWHe11 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{He})_{11}\). More... | |
| virtual const double | CEWHe22 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{He})_{22}\). More... | |
| virtual const double | CEWHe33 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{He})_{33}\). More... | |
| virtual const double | CEWHL111 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(1)})_{11}\). More... | |
| virtual const double | CEWHL122 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(1)})_{22}\). More... | |
| virtual const double | CEWHL133 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(1)})_{33}\). More... | |
| virtual const double | CEWHL311 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(3)})_{11}\). More... | |
| virtual const double | CEWHL322 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(3)})_{22}\). More... | |
| virtual const double | CEWHL333 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(3)})_{33}\). More... | |
| virtual const double | CEWHQ111 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{11}\). More... | |
| virtual const double | CEWHQ122 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{22}\). More... | |
| virtual const double | CEWHQ133 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{33}\). More... | |
| virtual const double | CEWHQ311 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{11}\). More... | |
| virtual const double | CEWHQ322 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{22}\). More... | |
| virtual const double | CEWHQ333 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{33}\). More... | |
| virtual const double | CEWHQd33 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(d)})_{33}\). More... | |
| virtual const double | CEWHu11 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{11}\). More... | |
| virtual const double | CEWHu22 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{22}\). More... | |
| virtual const double | CEWHu33 () const |
| Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{33}\). More... | |
| virtual const double | cgaga_HB (const double mu) const |
| The Higgs-basis coupling \(c_{\gamma\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual const double | cgg_HB (const double mu) const |
| The Higgs-basis coupling \(c_{gg}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual const double | cggEff_HB (const double mu) const |
| The effective Higgs-basis coupling \(c_{gg}^{Eff}\). (Similar to cgg_HB but including modifications of SM loops.) (See arXiv: 1505.00046 [hep-ph] document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual bool | CheckParameters (const std::map< std::string, double > &DPars) |
| A method to check if all the mandatory parameters for NPSMEFTd6 have been provided in model initialization. More... | |
| virtual const double | computeGammaTotalRatio () const |
| The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. More... | |
| virtual const double | cZBox_HB (const double mu) const |
| The Higgs-basis coupling \(c_{z\Box}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual const double | cZga_HB (const double mu) const |
| The Higgs-basis coupling \(c_{z\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual const double | cZZ_HB (const double mu) const |
| The Higgs-basis coupling \(c_{zz}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual const double | delta2sBRH3 (const double C1prod, const double C1Hxx) const |
| Quadratic contribution from the Higgs self-couplings modifications to the signal strength for \(\sigma \times BR(H\to xx)\) in the current model. More... | |
| virtual const double | delta2sH3 (const double C1) const |
| Quadratic contribution from the Higgs self-couplings modifications to the signal strength for an observable \(\sigma\) in the current model. More... | |
| virtual const double | delta_AFB_ee (const double pol_e, const double pol_p, const double s) const |
| virtual const double | delta_AFB_f (const Particle f, const double pol_e, const double pol_p, const double s) const |
| virtual const double | delta_Dsigma_f (const Particle f, const double pol_e, const double pol_p, const double s, const double cos) const |
| virtual const double | delta_mubbH_1 (const double sqrt_s) const |
| The SMEFT linear correction to the ratio \(\mu_{bbH}\) between the bbH production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_mubbH_2 (const double sqrt_s) const |
| The SMEFT quadratic correction to the ratio \(\mu_{bbH}\) between the bbH production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_muggH_1 (const double sqrt_s) const |
| The SMEFT linear correction to the ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_muggH_2 (const double sqrt_s) const |
| The SMEFT quadratic correction to the ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_mutH_1 (const double sqrt_s) const |
| The SMEFT linear correction to the ratio \(\mu_{tH}\) between the t-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_mutH_2 (const double sqrt_s) const |
| The SMEFT quadratic correction to the ratio \(\mu_{tH}\) between the t-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_muttH_1 (const double sqrt_s) const |
| The SMEFT linear correction to the ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_muttH_2 (const double sqrt_s) const |
| The SMEFT quadratic correction to the ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_muVBF_1 (const double sqrt_s) const |
| The SMEFT linear correction to the ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_muVBF_2 (const double sqrt_s) const |
| The SMEFT quadratic correction to the ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_muVH_1 (const double sqrt_s) const |
| The SMEFT linear correction to the ratio \(\mu_{VH}\) between the Z-Higgs and W-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_muVH_2 (const double sqrt_s) const |
| The SMEFT quadratic correction to the ratio \(\mu_{VH}\) between the Z-Higgs and W-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_muWH_1 (const double sqrt_s) const |
| The SMEFT linear correction to the ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_muWH_2 (const double sqrt_s) const |
| The SMEFT quadratic correction to the ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_muZH_1 (const double sqrt_s) const |
| The SMEFT linear correction to the ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_muZH_2 (const double sqrt_s) const |
| The SMEFT quadratic correction to the ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | delta_sigma_ee (const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const |
| virtual const double | delta_sigma_f (const Particle f, const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const |
| virtual const double | delta_sigma_had (const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const |
| virtual const double | delta_sigmaTot_ee (const double pol_e, const double pol_p, const double s) const |
| virtual const double | delta_sigmaTot_f (const Particle f, const double pol_e, const double pol_p, const double s) const |
| virtual const double | deltaa0 () const |
| The relative correction to the electromagnetic constant at zero momentum, \(\delta \alpha(0)/\alpha(0)\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltaa02 () const |
| The relative correction to the electromagnetic constant at zero momentum, \((\delta \alpha(0)/\alpha(0))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltaaMZ () const |
| The relative correction to the electromagnetic constant at the Z pole, \(\delta \alpha(M_Z^2)/\alpha(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltaaMZ2 () const |
| The relative correction to the electromagnetic constant at the Z pole, \((\delta \alpha(M_Z^2)/\alpha(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltaaSMZ () const |
| The relative correction to the strong coupling constant at the Z pole, \(\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltaaSMZ2 () const |
| The relative correction to the strong coupling constant at the Z pole, \((\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltacZ_HB (const double mu) const |
| The Higgs-basis coupling \(\delta c_z\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual const double | deltadxsdcoseeWWlvjjLEP2 (double sqrt_s, const int bin) const |
| The new physics contribution to the differential cross section in pb for \(e^+ e^- \to W^+ W^- \to lv jj \), with \( l= e,\mu \) for the 4 \( cos{\theta}\) bins defined in arXiv: 1606.06693 [hep-ph]. for the C.O.M. energies of 182.6 and 205.9 GeV. From arXiv: 1606.06693 [hep-ph]. More... | |
| virtual const double | deltaG1_hWW () const |
| The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\). More... | |
| virtual const double | deltaG1_hZA () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\). More... | |
| virtual const double | deltaG1_hZARatio () const |
| The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More... | |
| virtual const double | deltaG1_hZZ () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\). More... | |
| virtual const double | deltag1gaNP (const double mu) const |
| The new physics contribution to the anomalous triple gauge coupling \(g_{1,\gamma}\). More... | |
| virtual const double | deltag1ZNP (const double mu) const |
| The new physics contribution to the anomalous triple gauge coupling \(g_{1,Z}\). More... | |
| virtual const double | deltag1ZNPEff () const |
| The new physics contribution to the effective anomalous triple gauge coupling \(g_{1,Z}^{Eff}\) from arXiv: 1708.09079 [hep-ph]. More... | |
| virtual const double | deltaG2_hWW () const |
| The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\). More... | |
| virtual const double | deltaG2_hZA () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\). More... | |
| virtual const double | deltaG2_hZZ () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\). More... | |
| virtual const double | deltaG3_hWW () const |
| The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\). More... | |
| virtual const double | deltaG3_hZZ () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\). More... | |
| const double | deltag3G () const |
| The new physics contribution to the coupling of the effective interaction \(f_{ABC} G_{\mu\nu}^A G_{\nu\rho}^B G_{\rho\mu}^C\). More... | |
| gslpp::complex | deltaG_Aff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More... | |
| gslpp::complex | deltaG_Gff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More... | |
| virtual const double | deltaG_hAA () const |
| The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\). More... | |
| virtual const double | deltaG_hAARatio () const |
| The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More... | |
| gslpp::complex | deltaG_hAff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More... | |
| virtual gslpp::complex | deltaG_hff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\). More... | |
| gslpp::complex | deltaG_hGff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More... | |
| virtual const double | deltaG_hgg () const |
| The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\). More... | |
| virtual const double | deltaG_hggRatio () const |
| The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More... | |
| virtual const double | deltaG_hhhRatio () const |
| The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value. More... | |
| gslpp::complex | deltaG_hZff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More... | |
| gslpp::complex | deltaG_Zff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More... | |
| virtual const double | deltaGA_f (const Particle p) const |
| New physics contribution to the neutral-current axial-vector coupling \(g_A^f\). More... | |
| virtual const double | deltaGA_f_2 (const Particle p) const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the neutral-current vector coupling \(g_A^f\). More... | |
| virtual const double | deltaGamma_W () const |
| The new physics contribution to the total decay width of the \(W\) boson, \(\delta \Gamma_W\). More... | |
| virtual const double | deltaGamma_W_2 () const |
| virtual const double | deltaGamma_Wff (const Particle fi, const Particle fj) const |
| The new physics contribution to the decay width of the \(W\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\). More... | |
| virtual const double | deltaGamma_Wff_2 (const Particle fi, const Particle fj) const |
| const double | deltaGammaH2d2dRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2d2d)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2d2dRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2d2d)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2e2muRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2e 2\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2e2muRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2e 2\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2e2vRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2e2v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2e2vRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2e2v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2evRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2ev)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2evRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2ev)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2L2dRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2L2dRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2L2LRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2L2LRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2L2uRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2L2uRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2L2v2Ratio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2L2v2Ratio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2L2vRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2l2vRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2L2vRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2l2vRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2Lv2Ratio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2Lv2Ratio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2LvRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2LvRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2mu2vRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2\mu 2v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2mu2vRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2\mu 2v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2muvRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2\mu v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2muvRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2\mu v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2u2dRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2u2d)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2u2dRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2u2d)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2u2uRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2u2u)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2u2uRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2u2u)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2udRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2ud)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2udRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2ud)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2v2dRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2v2d)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2v2dRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2v2d)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2v2uRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2v2u)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2v2uRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2v2u)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2v2vRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2v2v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH2v2vRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 2v2v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4dRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4d)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4dRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4d)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4eRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4e)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4eRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4e)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4fRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4f)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4fRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4f)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4L2Ratio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4L2Ratio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4LRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4lRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4LRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4lRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4muRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4muRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4uRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4u)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4uRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4u)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4vRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaH4vRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to 4v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHbbRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHbbRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHccRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHccRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHevmuvRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to e\nu \mu\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHevmuvRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to e\nu \mu\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHgagaRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHgagaRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHggRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. More... | |
| const double | deltaGammaHggRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHll_vvorjjRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to l l \nu\nu, l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHll_vvorjjRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to l l \nu\nu, l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHlv_lvorjjRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to l \nu l \nu, l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHlv_lvorjjRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to l \nu l \nu, l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHlvjjRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHlvjjRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHLvudRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHLvudRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHLvvLRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHLvvLRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHmumuRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHmumuRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHtautauRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHtautauRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHudduRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to uddu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHudduRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to uddu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHWW4fRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHWW4fRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHWWRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHWWRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZgaRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZgaRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZZ4fRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZZ4fRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZZRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| const double | deltaGammaHZZRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| virtual const double | deltaGammaTotalRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. More... | |
| virtual const double | deltaGammaTotalRatio1noError () const |
| The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. Neglecting SM theory errors. More... | |
| virtual const double | deltaGammaTotalRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are quadratic in the effective Lagrangian coefficients. More... | |
| virtual const double | DeltaGF () const |
| New physics contribution to the Fermi constant. More... | |
| const double | deltaGL_f (const Particle p) const |
| New physics contribution to the neutral-current left-handed coupling \(g_L^f\). More... | |
| const double | deltaGL_f_2 (const Particle p) const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the left-handed coupling \(g_L^f\). More... | |
| virtual gslpp::complex | deltaGL_Wff (const Particle pbar, const Particle p) const |
| New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\). More... | |
| gslpp::complex | deltaGL_Wffh (const Particle pbar, const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_L}\gamma^mu f_L\). More... | |
| const double | deltaGL_Zffh (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_L}\gamma^mu f_L\). More... | |
| virtual const double | deltaGmu () const |
| The relative correction to the muon decay constant, \(\delta G_\mu/G_\mu\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltaGmu2 () const |
| The relative correction to the muon decay constant, \((\delta G_\mu/G_\mu)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| const double | deltaGR_f (const Particle p) const |
| New physics contribution to the neutral-current right-handed coupling \(g_R^f\). More... | |
| const double | deltaGR_f_2 (const Particle p) const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the right-handed coupling \(g_R^f\). More... | |
| virtual gslpp::complex | deltaGR_Wff (const Particle pbar, const Particle p) const |
| New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\). More... | |
| gslpp::complex | deltaGR_Wffh (const Particle pbar, const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_R}\gamma^mu f_R\). More... | |
| const double | deltaGR_Zffh (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_R}\gamma^mu f_R\). More... | |
| virtual const double | deltaGV_f (const Particle p) const |
| New physics contribution to the neutral-current vector coupling \(g_V^f\). More... | |
| virtual const double | deltaGV_f_2 (const Particle p) const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the neutral-current vector coupling \(g_V^f\). More... | |
| virtual const double | deltaGwd6 () const |
| The relative NP corrections to the width of the \(W\) boson, \(\delta \Gamma_W/\Gamma_W\). More... | |
| virtual const double | deltaGwd62 () const |
| The relative NP corrections to the width of the \(W\) boson squared, \((\delta \Gamma_W/\Gamma_W)^2\). More... | |
| virtual const double | deltaGzd6 () const |
| The relative NP corrections to the width of the \(Z\) boson, \(\delta \Gamma_Z/\Gamma_Z\). More... | |
| virtual const double | deltaGzd62 () const |
| The relative NP corrections to the width of the \(Z\) boson squared, \((\delta \Gamma_Z/\Gamma_Z)^2\). More... | |
| virtual const double | deltaH3L1 (double C1) const |
| The coefficient of the 1-loop linear term in the Higgs selfcoupling. More... | |
| virtual const double | deltaH3L2 (double C1) const |
| The coefficient of the 1-loop quadratic term in the Higgs selfcoupling. More... | |
| virtual const double | deltaKgammaNP (const double mu) const |
| The new physics contribution to the anomalous triple gauge coupling \(\kappa_{\gamma}\). More... | |
| virtual const double | deltaKgammaNPEff () const |
| The new physics contribution to the effective anomalous triple gauge coupling \(\kappa_{\gamma}^{Eff}\) from arXiv: 1708.09079 [hep-ph]. More... | |
| virtual const double | deltaKZNP (const double mu) const |
| The new physics contribution to the anomalous triple gauge coupling \(\kappa_{Z}\). More... | |
| virtual const double | deltamb () const |
| The relative correction to the mass of the \(b\) quark, \(\delta m_b/m_b\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltamb2 () const |
| The relative correction to the mass of the \(b\) quark squared, \((\delta m_b/m_b)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltamc () const |
| The relative correction to the mass of the \(c\) quark, \(\delta m_c/m_c\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltamc2 () const |
| The relative correction to the mass of the \(c\) quark squared, \((\delta m_c/m_c)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltaMh () const |
| The relative correction to the mass of the \(H\) boson, \(\delta M_H/M_H\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltaMh2 () const |
| The relative correction to the mass of the \(H\) boson squared, \((\delta M_H/M_H)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| const double | deltaMLL2_f (const Particle f, const double s, const double t) const |
| const double | deltaMLR2_f (const Particle f, const double s) const |
| const double | deltaMLR2t_e (const double t) const |
| const double | deltaMRL2_f (const Particle f, const double s) const |
| const double | deltaMRL2t_e (const double t) const |
| const double | deltaMRR2_f (const Particle f, const double s, const double t) const |
| virtual const double | deltamt () const |
| The relative correction to the mass of the \(t\) quark, \(\delta m_t/m_t\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltamt2 () const |
| The relative correction to the mass of the \(t\) quark squared, \((\delta m_t/m_t)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltamtau () const |
| The relative correction to the mass of the \(\tau\) lepton, \(\delta m_\tau/m_\tau\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltamtau2 () const |
| The relative correction to the mass of the \(\tau\) lepton squared, \((\delta m_\tau/m_\tau)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltaMw () const |
| The relative correction to the mass of the \(W\) boson, \(\delta M_W/M_W\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltaMw2 () const |
| The relative correction to the mass of the \(W\) boson squared, \((\delta M_W/M_W)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltaMwd6 () const |
| The relative NP corrections to the mass of the \(W\) boson, \(\delta M_W/M_W\). More... | |
| virtual const double | deltaMwd62 () const |
| The relative NP corrections to the mass of the \(W\) boson squared, \((\delta M_W/M_W)^2\). More... | |
| virtual const double | deltaMwd6_2 () const |
| The relative \(\mathcal{O}(\Lambda^{-4})\) NP corrections to the mass of the \(W\) boson, \(\Delta M_W^{(2)}\). More... | |
| virtual const double | deltaMz () const |
| The relative correction to the mass of the \(Z\) boson, \(\delta M_Z/M_Z\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltaMz2 () const |
| The relative correction to the mass of the \(Z\) boson squared, \((\delta M_Z/M_Z)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual const double | deltaxseeWW4fLEP2 (double sqrt_s, const int fstate) const |
| The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to 4f \), with \( 4f = 0 (jjjj), 1 (e v jj), 2 (mu v jj), 3 (tau v jj), 4 (e v e v), 5 (mu v mu v), 6 (tau v tau v), 7 (e v mu v), 8 (e v tau v), 9 (mu v tau v), 10 (l v jj), 11 (l v l v) \) the different fermion final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. More... | |
| virtual const double | deltaxseeWWtotLEP2 (double sqrt_s) const |
| The new physics contribution to the total cross section in pb for \(e^+ e^- \to W^+ W^-\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. More... | |
| virtual const double | deltayb_HB (const double mu) const |
| The Higgs-basis coupling \(\delta y_b\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual const double | deltayc_HB (const double mu) const |
| The Higgs-basis coupling \(\delta y_c\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual const double | deltaymu_HB (const double mu) const |
| The Higgs-basis coupling \(\delta y_\mu\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual const double | deltays_HB (const double mu) const |
| The Higgs-basis coupling \(\delta y_s\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual const double | deltayt_HB (const double mu) const |
| The Higgs-basis coupling \(\delta y_t\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual const double | deltaytau_HB (const double mu) const |
| The Higgs-basis coupling \(\delta y_\tau\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual const double | dxsdcoseeWWlvjjLEP2 (double sqrt_s, const int bin) const |
| The differential cross section in pb for \(e^+ e^- \to W^+ W^- \to lv jj \), with \( l= e,\mu \) for the 4 \( cos{\theta}\) bins defined in arXiv: 1606.06693 [hep-ph]. for the C.O.M. energies of 182.6 and 205.9 GeV. From arXiv: 1606.06693 [hep-ph]. More... | |
| virtual const double | dxseeWWdcos (double sqrt_s, double cos) const |
| The differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\), as a function of the \(W\) polar angle. More... | |
| virtual const double | dxseeWWdcosBin (double sqrt_s, double cos1, double cos2) const |
| The integral of differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\) in a given bin of the \(W\) polar angle. More... | |
| gslpp::complex | f_triangle (double tau) const |
| Loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings. More... | |
| bool | flagCHWpCHB () const |
| If True, uses the coefficient CHWpCHW instead of the sum CiHW+CiHB. More... | |
| gslpp::complex | g_triangle (double tau) const |
| Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| const double | GammaH2d2dRatio () const |
| The ratio of the \(\Gamma(H\to 2d2d)\) in the current model and in the Standard Model. More... | |
| const double | GammaH2e2muRatio () const |
| The ratio of the \(\Gamma(H\to 2e 2\mu)\) in the current model and in the Standard Model. More... | |
| const double | GammaH2e2vRatio () const |
| The ratio of the \(\Gamma(H\to 2e2v)\) in the current model and in the Standard Model. More... | |
| const double | GammaH2evRatio () const |
| The ratio of the \(\Gamma(H\to 2ev)\) in the current model and in the Standard Model. More... | |
| const double | GammaH2L2dRatio () const |
| The ratio of the \(\Gamma(H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| const double | GammaH2L2LRatio () const |
| The ratio of the \(\Gamma(H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| const double | GammaH2L2uRatio () const |
| The ratio of the \(\Gamma(H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| const double | GammaH2L2v2Ratio () const |
| The ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. More... | |
| const double | GammaH2L2vRatio () const |
| The ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| const double | GammaH2l2vRatio () const |
| The ratio of the \(\Gamma(H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. More... | |
| const double | GammaH2Lv2Ratio () const |
| The ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. More... | |
| const double | GammaH2LvRatio () const |
| The ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| const double | GammaH2mu2vRatio () const |
| The ratio of the \(\Gamma(H\to 2\mu 2v)\) in the current model and in the Standard Model. More... | |
| const double | GammaH2muvRatio () const |
| The ratio of the \(\Gamma(H\to 2\mu v)\) in the current model and in the Standard Model. More... | |
| const double | GammaH2u2dRatio () const |
| The ratio of the \(\Gamma(H\to 2u2d)\) in the current model and in the Standard Model. More... | |
| const double | GammaH2u2uRatio () const |
| The ratio of the \(\Gamma(H\to 2u2u)\) in the current model and in the Standard Model. More... | |
| const double | GammaH2udRatio () const |
| The ratio of the \(\Gamma(H\to 2ud)\) in the current model and in the Standard Model. More... | |
| const double | GammaH2v2dRatio () const |
| The ratio of the \(\Gamma(H\to 2v2d)\) in the current model and in the Standard Model. More... | |
| const double | GammaH2v2uRatio () const |
| The ratio of the \(\Gamma(H\to 2v2u)\) in the current model and in the Standard Model. More... | |
| const double | GammaH2v2vRatio () const |
| The ratio of the \(\Gamma(H\to 2v2v)\) in the current model and in the Standard Model. More... | |
| const double | GammaH4dRatio () const |
| The ratio of the \(\Gamma(H\to 4d)\) in the current model and in the Standard Model. More... | |
| const double | GammaH4eRatio () const |
| The ratio of the \(\Gamma(H\to 4e)\) in the current model and in the Standard Model. More... | |
| const double | GammaH4fRatio () const |
| The ratio of the \(\Gamma(H\to 4f)\) in the current model and in the Standard Model. More... | |
| const double | GammaH4L2Ratio () const |
| The ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. More... | |
| const double | GammaH4LRatio () const |
| The ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| const double | GammaH4lRatio () const |
| The ratio of the \(\Gamma(H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. More... | |
| const double | GammaH4muRatio () const |
| The ratio of the \(\Gamma(H\to 4\mu)\) in the current model and in the Standard Model. More... | |
| const double | GammaH4uRatio () const |
| The ratio of the \(\Gamma(H\to 4u)\) in the current model and in the Standard Model. More... | |
| const double | GammaH4vRatio () const |
| The ratio of the \(\Gamma(H\to 4v)\) in the current model and in the Standard Model. More... | |
| const double | GammaHbbRatio () const |
| The ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. More... | |
| const double | GammaHccRatio () const |
| The ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. More... | |
| const double | GammaHevmuvRatio () const |
| The ratio of the \(\Gamma(H\to e\nu \mu\nu)\) in the current model and in the Standard Model. More... | |
| const double | GammaHgagaRatio () const |
| The ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. More... | |
| const double | GammaHggRatio () const |
| The ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. More... | |
| const double | GammaHll_vvorjjRatio () const |
| The ratio of the \(\Gamma(H\to l l \nu\nu, l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. More... | |
| const double | GammaHlv_lvorjjRatio () const |
| The ratio of the \(\Gamma(H\to l \nu l \nu, l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. More... | |
| const double | GammaHlvjjRatio () const |
| The ratio of the \(\Gamma(H\to l l j j)\) ( \(l=e,\mu@f,~~j\not=b$) in the current model and in the Standard Model. @return \)\Gamma(H\to l l j j) \(/\)\Gamma(H\to l l j j)_{\mathrm{SM}} \( */ const double GammaHlljjRatio() const; /** @brief The new physics contribution to the ratio of the \)\Gamma(H\to l l j j) \( (\)l=e,\mu,~~j\not=b \() in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) @return \)\delta \Gamma(H\to l l j j) \(/\)\Gamma(H\to l l j j)_{\mathrm{SM}} \( */ const double deltaGammaHlljjRatio1() const; /** @brief The new physics contribution to the ratio of the \)\Gamma(H\to l l j j) \( (\)l=e,\mu,~~j\not=b \() in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) @return \)\delta \Gamma(H\to l l j j) \(/\)\Gamma(H\to l l j j)_{\mathrm{SM}} \( */ const double deltaGammaHlljjRatio2() const; /** @brief The ratio of the Br\)(H\to l l j j) \( (\)l=e,\mu,~~j\not=b \() in the current model and in the Standard Model. @return Br\)(H\to l l j j) \(/Br\)(H\to l l j j)_{\mathrm{SM}} \( */ virtual const double BrHlljjRatio() const; /** @brief The ratio of the \)\Gamma(H\to l \nu j j) \( (\)l=e,\mu@f,~~j\not=b$) in the current model and in the Standard Model. More... | |
| const double | GammaHLvudRatio () const |
| The ratio of the \(\Gamma(H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| const double | GammaHLvvLRatio () const |
| The ratio of the \(\Gamma(H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. More... | |
| const double | GammaHmumuRatio () const |
| The ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. More... | |
| const double | GammaHtautauRatio () const |
| The ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. More... | |
| const double | GammaHudduRatio () const |
| The ratio of the \(\Gamma(H\to uddu)\) in the current model and in the Standard Model. More... | |
| const double | GammaHWW4fRatio () const |
| The ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| const double | GammaHWWRatio () const |
| The ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. More... | |
| const double | GammaHZgaRatio () const |
| The ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. More... | |
| const double | GammaHZZ4fRatio () const |
| The ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| const double | GammaHZZRatio () const |
| The ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. More... | |
| virtual const double | GammaW () const |
| The total width of the \(W\) boson, \(\Gamma_W\). More... | |
| virtual const double | GammaW (const Particle fi, const Particle fj) const |
| A partial decay width of the \(W\) boson decay into a SM fermion pair. More... | |
| const double | getCed_1123 () const |
| Return NP coeff Ced_1123. More... | |
| const double | getCed_2223 () const |
| Return NP coeff Ced_2223. More... | |
| const double | getCeu_1133 () const |
| Return NP coeff Ceu_1133. More... | |
| const double | getCeu_2233 () const |
| Return NP coeff Ceu_2233. More... | |
| const double | getCHe_11 () const |
| Return NP coeff CHe_11. More... | |
| const double | getCHe_22 () const |
| Return NP coeff CHe_22. More... | |
| const double | getCHL1_11 () const |
| Return NP coeff CHL1_11. More... | |
| const double | getCHL1_22 () const |
| Return NP coeff CHL1_22. More... | |
| const double | getCHL3_11 () const |
| Return NP coeff CHL3_11. More... | |
| const double | getCHL3_22 () const |
| Return NP coeff CHL3_22. More... | |
| const double | getCLd_1123 () const |
| Return NP coeff CLd_1123. More... | |
| const double | getCLd_2223 () const |
| Return NP coeff CLd_2223. More... | |
| const double | getCLd_3323 () const |
| Return NP coeff CLd_3323. More... | |
| const double | getCLedQ_11 () const |
| Return NP coeff CLedq_11. More... | |
| const double | getCLedQ_22 () const |
| Return NP coeff CLedq_22. More... | |
| const double | getCLQ1_1123 () const |
| Return NP coeff CLQ1_1123. More... | |
| const double | getCLQ1_2223 () const |
| Return NP coeff CLQ1_2223. More... | |
| const double | getCLQ1_3323 () const |
| Return NP coeff CLQ1_3323. More... | |
| const double | getCLQ3_1123 () const |
| Return NP coeff CLQ3_1123. More... | |
| const double | getCLQ3_2223 () const |
| Return NP coeff CLQ3_2223. More... | |
| const double | getCLQ3_3323 () const |
| Return NP coeff CLQ3_3323. More... | |
| const double | getCLu_1133 () const |
| Return NP coeff CLu_1133. More... | |
| const double | getCLu_2233 () const |
| Return NP coeff CLu_2233. More... | |
| const double | getCpLedQ_11 () const |
| Return NP coeff CpLedq_11. More... | |
| const double | getCpLedQ_22 () const |
| Return NP coeff CpLedq_22. More... | |
| const double | getCQe_2311 () const |
| Return NP coeff CQe_2322. More... | |
| const double | getCQe_2322 () const |
| Return NP coeff CQe_2322. More... | |
| const double | getLambda_NP () const |
| Return Lambda_NP. More... | |
| virtual NPSMEFTd6Matching & | getMatching () const |
| A method to get the Matching object for this model. More... | |
| bool | hatCis () const |
| If True, explicitly defines the 8 'hat' coefficients in the EWPOs (Z-couplings, dGf, W-width) More... | |
| gslpp::complex | I_triangle_1 (double tau, double lambda) const |
| Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| gslpp::complex | I_triangle_2 (double tau, double lambda) const |
| Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| virtual const double | intDMLL2eus2 (const double s, const double t0, const double t1) const |
| virtual const double | intDMLR2etildest2 (const double s, const double t0, const double t1) const |
| virtual const double | intDMLR2ets2 (const double s, const double t0, const double t1) const |
| virtual const double | intDMRL2etildest2 (const double s, const double t0, const double t1) const |
| virtual const double | intDMRL2ets2 (const double s, const double t0, const double t1) const |
| virtual const double | intDMRR2eus2 (const double s, const double t0, const double t1) const |
| virtual const double | intMeeLL2SMus2 (const double s, const double t0, const double t1) const |
| virtual const double | intMeeLR2SMts2 (const double s, const double t0, const double t1) const |
| virtual const double | intMeeLRtilde2SMst2 (const double s, const double t0, const double t1) const |
| virtual const double | intMeeRR2SMus2 (const double s, const double t0, const double t1) const |
| virtual const double | kappaAeff () const |
| The effective coupling \(\kappa_{A,eff}=\sqrt{\Gamma_{HAA}/\Gamma_{HAA}^{SM}}\). More... | |
| virtual const double | kappabeff () const |
| The effective coupling \(\kappa_{b,eff}=\sqrt{\Gamma_{Hbb}/\Gamma_{Hbb}^{SM}}\). More... | |
| virtual const double | kappaceff () const |
| The effective coupling \(\kappa_{c,eff}=\sqrt{\Gamma_{Hcc}/\Gamma_{Hcc}^{SM}}\). More... | |
| virtual const double | kappaGeff () const |
| The effective coupling \(\kappa_{G,eff}=\sqrt{\Gamma_{HGG}/\Gamma_{HGG}^{SM}}\). More... | |
| virtual const double | kappamueff () const |
| The effective coupling \(\kappa_{\mu,eff}=\sqrt{\Gamma_{H\mu\mu}/\Gamma_{H\mu\mu}^{SM}}\). More... | |
| virtual const double | kappataueff () const |
| The effective coupling \(\kappa_{\tau,eff}=\sqrt{\Gamma_{H\tau\tau}/\Gamma_{H\tau\tau}^{SM}}\). More... | |
| virtual const double | kappaWeff () const |
| The effective coupling \(\kappa_{W,eff}=\sqrt{\Gamma_{HWW}/\Gamma_{HWW}^{SM}}\). More... | |
| virtual const double | kappaZAeff () const |
| The effective coupling \(\kappa_{ZA,eff}=\sqrt{\Gamma_{HZA}/\Gamma_{HZA}^{SM}}\). More... | |
| virtual const double | kappaZeff () const |
| The effective coupling \(\kappa_{Z,eff}=\sqrt{\Gamma_{HZZ}/\Gamma_{HZZ}^{SM}}\). More... | |
| virtual const double | lambdaZNP (const double mu) const |
| The new physics contribution to the anomalous triple gauge coupling \(\lambda_{Z}\). More... | |
| virtual const double | lambz_HB (const double mu) const |
| The Higgs-basis coupling \(\lambda_{z}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual const double | mueeHvv (double sqrt_s, double Pol_em, double Pol_ep) const |
| The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueeHvvPol (double sqrt_s, double Pol_em, double Pol_ep) const |
| The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueettH (double sqrt_s, double Pol_em, double Pol_ep) const |
| The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueettHPol (double sqrt_s, double Pol_em, double Pol_ep) const |
| The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueeWBF (double sqrt_s, double Pol_em, double Pol_ep) const |
| The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueeWW (double sqrt_s, double Pol_em, double Pol_ep) const |
| The ratio \(\mu_{eeWW}\) between the \( e^{+}e^{-}\to W^{+}W^{-} \) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueeWWPol (double sqrt_s, double Pol_em, double Pol_ep) const |
| The ratio \(\mu_{eeWW}\) between the \( e^{+}e^{-}\to W^{+}W^{-} \) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueeZBF (double sqrt_s, double Pol_em, double Pol_ep) const |
| The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueeZBFPol (double sqrt_s, double Pol_em, double Pol_ep) const |
| The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueeZH (double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeZH}\) between the \(e^{+}e^{-}\to ZH\) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueeZHPol (double sqrt_s, double Pol_em, double Pol_ep) const |
| The ratio \(\mu_{eeZH}\) between the \( e^{+}e^{-}\to ZH \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueeZllH (double sqrt_s, double Pol_em, double Pol_ep) const |
| The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueeZllHPol (double sqrt_s, double Pol_em, double Pol_ep) const |
| The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueeZqqH (double sqrt_s, double Pol_em, double Pol_ep) const |
| The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueeZqqHPol (double sqrt_s, double Pol_em, double Pol_ep) const |
| The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muepWBF (double sqrt_s) const |
| The ratio \(\mu_{epWBF}\) between the \( e^{-} p\to \nu j H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muepZBF (double sqrt_s) const |
| The ratio \(\mu_{epZBF}\) between the \( e^{-} p\to e^{-} j H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muggH (double sqrt_s) const |
| The ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muggHbb (double sqrt_s) const |
| The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual const double | muggHgaga (double sqrt_s) const |
| The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual const double | muggHH (double sqrt_s) const |
| The ratio \(\mu_{ggHH}\) between the gluon-gluon fusion di-Higgs production cross-section in the current model and in the Standard Model. (From arXiv: 1502.00539 [hpe-ph].) More... | |
| virtual const double | muggHmumu (double sqrt_s) const |
| The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual const double | muggHpttH (double sqrt_s) const |
| The ratio \(\mu_{ggH+ttH}\) between the sum of gluon-gluon fusion and t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muggHtautau (double sqrt_s) const |
| The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual const double | muggHWW (double sqrt_s) const |
| The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muggHWW2l2v (double sqrt_s) const |
| The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual const double | muggHZga (double sqrt_s) const |
| The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual const double | muggHZZ (double sqrt_s) const |
| The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muggHZZ4l (double sqrt_s) const |
| The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual const double | mummH (double sqrt_s) const |
| The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mummHmm (double sqrt_s) const |
| The ratio \(\mu_{\mu\mu H\mu\mu}\) between the \(\sigma(\mu \mu \to H \mu \mu)}\) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mummHNWA (double sqrt_s) const |
| The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model, in the narrow width approximation. More... | |
| virtual const double | mummHvv (double sqrt_s) const |
| The ratio \(\mu_{\mu\mu H\nu\nu}\) between the \(\sigma(\mu \mu \to H \nu \nu)}\) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mummttH (double sqrt_s) const |
| The ratio \(\mu_{\mu\mu ttH}\) between the \(\sigma(\mu \mu \to t\bar{t} H )}\) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mummZH (double sqrt_s) const |
| The ratio \(\mu_{\mu\mu ZH}\) between the \(\sigma(\mu \mu \to Z H)}\) production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mupTVppWZ (double sqrt_s, double pTV1, double pTV2) const |
| The number of events in \( p p \to WZ\) in a given \(p_{TV}\) bin, normalized to the SM prediction. From arXiv: 1712.01310 [hep-ph] and private communication. Implemented only in NPSMEFTd6 class. More... | |
| virtual const double | mutHq (double sqrt_s) const |
| The ratio \(\mu_{tHq}\) between the t-q-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muTHUggHbb (double sqrt_s) const |
| The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUggHgaga (double sqrt_s) const |
| The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual const double | muTHUggHmumu (double sqrt_s) const |
| The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUggHtautau (double sqrt_s) const |
| The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUggHWW (double sqrt_s) const |
| The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUggHWW2l2v (double sqrt_s) const |
| The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUggHZga (double sqrt_s) const |
| The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUggHZgamumu (double sqrt_s) const |
| The ratio \(\mu_{ggH,Z\gamma\to \gamma 2\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\to \gamma 2\mu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUggHZZ (double sqrt_s) const |
| The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUggHZZ4l (double sqrt_s) const |
| The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUggHZZ4mu (double sqrt_s) const |
| The ratio \(\mu_{ggH,ZZ\to 4\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4\mu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUttHbb (double sqrt_s) const |
| The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUttHgaga (double sqrt_s) const |
| The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual const double | muTHUttHmumu (double sqrt_s) const |
| The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUttHtautau (double sqrt_s) const |
| The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUttHWW (double sqrt_s) const |
| The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUttHWW2l2v (double sqrt_s) const |
| The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUttHZga (double sqrt_s) const |
| The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUttHZZ (double sqrt_s) const |
| The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUttHZZ4l (double sqrt_s) const |
| The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVBFBRinv (double sqrt_s) const |
| The ratio \(\mu_{VBF}\) between the VBF production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio. More... | |
| virtual const double | muTHUVBFHbb (double sqrt_s) const |
| The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVBFHgaga (double sqrt_s) const |
| The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVBFHinv (double sqrt_s) const |
| The ratio \(\mu_{VBF,inv}\) between the VBF production cross-section with subsequent decay into invisible states in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVBFHmumu (double sqrt_s) const |
| The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVBFHtautau (double sqrt_s) const |
| The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVBFHWW (double sqrt_s) const |
| The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVBFHWW2l2v (double sqrt_s) const |
| The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVBFHZga (double sqrt_s) const |
| The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVBFHZZ (double sqrt_s) const |
| The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVBFHZZ4l (double sqrt_s) const |
| The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVHbb (double sqrt_s) const |
| The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVHBRinv (double sqrt_s) const |
| The ratio \(\mu_{VH}\) between the VH production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio. More... | |
| virtual const double | muTHUVHgaga (double sqrt_s) const |
| The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVHinv (double sqrt_s) const |
| The ratio \(\mu_{VH,inv}\) between the VH production cross-section with subsequent decay into invisible states in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVHmumu (double sqrt_s) const |
| The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVHtautau (double sqrt_s) const |
| The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVHWW (double sqrt_s) const |
| The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVHWW2l2v (double sqrt_s) const |
| The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVHZga (double sqrt_s) const |
| The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVHZZ (double sqrt_s) const |
| The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUVHZZ4l (double sqrt_s) const |
| The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUWHbb (double sqrt_s) const |
| The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUWHgaga (double sqrt_s) const |
| The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual const double | muTHUWHmumu (double sqrt_s) const |
| The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUWHtautau (double sqrt_s) const |
| The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUWHWW (double sqrt_s) const |
| The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUWHWW2l2v (double sqrt_s) const |
| The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUWHZga (double sqrt_s) const |
| The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUWHZZ (double sqrt_s) const |
| The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUWHZZ4l (double sqrt_s) const |
| The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUZHbb (double sqrt_s) const |
| The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUZHgaga (double sqrt_s) const |
| The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual const double | muTHUZHmumu (double sqrt_s) const |
| The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUZHtautau (double sqrt_s) const |
| The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUZHWW (double sqrt_s) const |
| The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUZHWW2l2v (double sqrt_s) const |
| The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUZHZga (double sqrt_s) const |
| The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUZHZZ (double sqrt_s) const |
| The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muTHUZHZZ4l (double sqrt_s) const |
| The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual const double | muttH (double sqrt_s) const |
| The ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muttHbb (double sqrt_s) const |
| The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual const double | muttHgaga (double sqrt_s) const |
| The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual const double | muttHgagaZeeboost (const double sqrt_s) const |
| The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H\to b\bar{b}\), \(Z\to e^+e^-\) channel channel in the current model and in the Standard Model. More... | |
| virtual const double | muttHmumu (double sqrt_s) const |
| The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual const double | muttHtautau (double sqrt_s) const |
| The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual const double | muttHWW (double sqrt_s) const |
| The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muttHWW2l2v (double sqrt_s) const |
| The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual const double | muttHZbbboost (double sqrt_s) const |
| The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H,Z\to b\bar{b}\) channel in the current model and in the Standard Model. More... | |
| virtual const double | muttHZga (double sqrt_s) const |
| The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual const double | muttHZZ (double sqrt_s) const |
| The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muttHZZ4l (double sqrt_s) const |
| The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual const double | muVBF (double sqrt_s) const |
| The ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muVBFgamma (double sqrt_s) const |
| The ratio \(\mu_{VBF+\gamma}\) between the vector-boson fusion Higgs production cross-section in association with a hard photon in the current model and in the Standard Model. More... | |
| virtual const double | muVBFHbb (double sqrt_s) const |
| The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual const double | muVBFHgaga (double sqrt_s) const |
| The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual const double | muVBFHmumu (double sqrt_s) const |
| The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual const double | muVBFHtautau (double sqrt_s) const |
| The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual const double | muVBFHWW (double sqrt_s) const |
| The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muVBFHWW2l2v (double sqrt_s) const |
| The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual const double | muVBFHZga (double sqrt_s) const |
| The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual const double | muVBFHZZ (double sqrt_s) const |
| The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muVBFHZZ4l (double sqrt_s) const |
| The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual const double | muVBFpVH (double sqrt_s) const |
| The ratio \(\mu_{VBF+VH}\) between the sum of VBF and WH+ZH associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muVH (double sqrt_s) const |
| The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muVHbb (double sqrt_s) const |
| The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual const double | muVHgaga (double sqrt_s) const |
| The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual const double | muVHmumu (double sqrt_s) const |
| The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual const double | muVHpT250 (double sqrt_s) const |
| The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model, with \(p_{T,H}>250\) GeV. More... | |
| virtual const double | muVHtautau (double sqrt_s) const |
| The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual const double | muVHWW (double sqrt_s) const |
| The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muVHWW2l2v (double sqrt_s) const |
| The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual const double | muVHZga (double sqrt_s) const |
| The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual const double | muVHZZ (double sqrt_s) const |
| The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muVHZZ4l (double sqrt_s) const |
| The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual const double | muWH (double sqrt_s) const |
| The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muWHbb (double sqrt_s) const |
| The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual const double | muWHgaga (double sqrt_s) const |
| The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual const double | muWHmumu (double sqrt_s) const |
| The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual const double | muWHpT250 (double sqrt_s) const |
| The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model, with \(p_{T,H}>250\) GeV. More... | |
| virtual const double | muWHtautau (double sqrt_s) const |
| The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual const double | muWHWW (double sqrt_s) const |
| The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muWHWW2l2v (double sqrt_s) const |
| The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual const double | muWHZga (double sqrt_s) const |
| The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual const double | muWHZZ (double sqrt_s) const |
| The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muWHZZ4l (double sqrt_s) const |
| The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual const double | muZH (double sqrt_s) const |
| The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muZHbb (double sqrt_s) const |
| The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual const double | muZHgaga (double sqrt_s) const |
| The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual const double | muZHmumu (double sqrt_s) const |
| The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual const double | muZHpT250 (double sqrt_s) const |
| The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model, with \(p_{T,H}>250\) GeV. More... | |
| virtual const double | muZHtautau (double sqrt_s) const |
| The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual const double | muZHWW (double sqrt_s) const |
| The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muZHWW2l2v (double sqrt_s) const |
| The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual const double | muZHZga (double sqrt_s) const |
| The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual const double | muZHZZ (double sqrt_s) const |
| The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual const double | muZHZZ4l (double sqrt_s) const |
| The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual const double | Mw () const |
| The mass of the \(W\) boson, \(M_W\). More... | |
| virtual const double | NevLHCppee13 (const int i_bin) const |
| Number of di-electron events at the LHC at 13 TeV. More... | |
| virtual const double | NevLHCppenu13 (const int i_bin) const |
| Number of mono-electron events at the LHC at 13 TeV. More... | |
| virtual const double | NevLHCppmumu13 (const int i_bin) const |
| Number of di-muon events at the LHC at 13 TeV. More... | |
| virtual const double | NevLHCppmunu13 (const int i_bin) const |
| Number of mono-muon events at the LHC at 13 TeV. More... | |
| virtual const double | NevLHCpptaunu13 (const int i_bin) const |
| Number of mono-tau events at the LHC at 13 TeV. More... | |
| virtual const double | NevLHCpptautau13 (const int i_bin) const |
| Number of di-tau events at the LHC at 13 TeV. More... | |
| NPSMEFTd6 (const bool FlagLeptonUniversal_in=false, const bool FlagQuarkUniversal_in=false) | |
| Constructor. More... | |
| virtual const double | obliqueS () const |
| The oblique parameter \(S\). (Simplified implementation. Contribution only from \(O_{HWB}\).) More... | |
| virtual const double | obliqueT () const |
| The oblique parameter \(T\). (Simplified implementation. Contribution only from \(O_{HD}\).) More... | |
| virtual const double | obliqueU () const |
| The oblique parameter \(U\). More... | |
| virtual const double | obliqueW () const |
| The oblique parameter \(W\). (Simplified implementation. Contribution only from \(O_{2W}\).) More... | |
| virtual const double | obliqueY () const |
| The oblique parameter \(Y\). (Simplified implementation. Contribution only from \(O_{2B}\).) More... | |
| virtual int | OutputOrder () const |
| Type of contributions to be included in the EWPOs. Takes a numerica values depending on the choice. More... | |
| virtual bool | PostUpdate () |
| The post-update method for NPSMEFTd6. More... | |
| virtual const double | ppZHprobe (double sqrt_s) const |
| The direction constrained by \( p p \to Z H\) in the boosted regime, \(g_p^Z\). From arXiv:1807.01796 and the contribution to FCC CDR Vol 1. Implemented only in NPSMEFTd6 class. More... | |
| virtual bool | RGd6SMEFTlogs () |
| A function to apply the 1st leading log corrections to the Wilson coefficients, according to the d6 SMEFT RGEs. More... | |
| virtual const double | RWc () const |
| The ratio \( R_{W,c}=\Gamma(W\to c + X)/\Gamma(W\to had) \). More... | |
| virtual const double | RWlilj (const Particle li, const Particle lj) const |
| The lepton universality ratio \(R_{W,l_i/l_j)=\Gamma(W\to l_i \nu_i)/\Gamma(W\to l_j \nu_j)\). More... | |
| virtual const double | RZlilj (const Particle li, const Particle lj) const |
| The lepton universality ratio \(R_{Z,l_i/l_j)=\Gamma(Z\to l_i^+ l_i^-)/\Gamma(Z\to l_j^+ l_j^-)\). More... | |
| virtual bool | setFlag (const std::string name, const bool value) |
| A method to set a flag of NPSMEFTd6. More... | |
| virtual const double | sigmaSM_ee (const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const |
| virtual const double | STXS0_qqH (double sqrt_s) const |
| The STXS0 bin \(pp \to H qq\). More... | |
| virtual const double | STXS12_BrH4lRatio () const |
| The STXS BR \( H \to 4l \), \(l=e,\mu\). More... | |
| virtual const double | STXS12_BrHbbRatio () const |
| The STXS BR \( H \to bb \). More... | |
| virtual const double | STXS12_BrHevmuvRatio () const |
| The STXS BR \( H \to e\nu \mu\nu \). More... | |
| virtual const double | STXS12_BrHgagaRatio () const |
| The STXS BR \( H \to \gamma \gamma \). More... | |
| virtual const double | STXS12_ggH_mjj0_350_pTH0_60_Nj2 (double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~m_{jj}[GeV]<350,~p_{TH} [GeV]<60\). More... | |
| virtual const double | STXS12_ggH_mjj0_350_pTH120_200_Nj2 (double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~m_{jj}[GeV]<350,~120<p_{TH} [GeV]<200\). More... | |
| virtual const double | STXS12_ggH_mjj0_350_pTH60_120_Nj2 (double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~m_{jj}[GeV]<350,~60<p_{TH} [GeV]<120\). More... | |
| virtual const double | STXS12_ggH_mjj350_700_pTH0_200_ptHjj0_25_Nj2 (double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH} [GeV]<200,~p_{THjj}[GeV]<25\). More... | |
| virtual const double | STXS12_ggH_mjj350_700_pTH0_200_ptHjj25_Inf_Nj2 (double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH} [GeV]<200,~25<p_{THjj}[GeV]\). More... | |
| virtual const double | STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj0_25_Nj2 (double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200,~p_{THjj}[GeV]<25\). More... | |
| virtual const double | STXS12_ggH_mjj700_Inf_pTH0_200_ptHjj25_Inf_Nj2 (double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200,~25<p_{THjj}[GeV]\). More... | |
| virtual const double | STXS12_ggH_pTH0_10_Nj0 (double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j=0,~p_{TH} [GeV]<10\). More... | |
| virtual const double | STXS12_ggH_pTH0_60_Nj1 (double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j = 1,~p_{TH} [GeV]<60\). More... | |
| virtual const double | STXS12_ggH_pTH10_Inf_Nj0 (double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j=0,~10<p_{TH} [GeV]\). More... | |
| virtual const double | STXS12_ggH_pTH120_200_Nj1 (double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j = 1,~120<p_{TH} [GeV]<200\). More... | |
| virtual const double | STXS12_ggH_pTH200_300_Nj01 (double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j\leq 1,~200<p_{TH} [GeV]<300\). More... | |
| virtual const double | STXS12_ggH_pTH300_450_Nj01 (double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j\leq 1,~300<p_{TH} [GeV]<450\). More... | |
| virtual const double | STXS12_ggH_pTH450_650_Nj01 (double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j\leq 1,~450<p_{TH} [GeV]<650\). More... | |
| virtual const double | STXS12_ggH_pTH60_120_Nj1 (double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j = 1,~60<p_{TH} [GeV]<120\). More... | |
| virtual const double | STXS12_ggH_pTH650_Inf_Nj01 (double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j\leq 1,650<p_{TH} [GeV]\). More... | |
| virtual const double | STXS12_ggHll_pTV0_75 (double sqrt_s) const |
| The STXS bin \(gg \to H\ell\ell\), \(p_{TV}[GeV]<75\). More... | |
| virtual const double | STXS12_ggHll_pTV150_250_Nj0 (double sqrt_s) const |
| The STXS bin \(gg \to H\ell\ell\), \(N_j = 0,~150<p_{TV}[GeV]<250\). More... | |
| virtual const double | STXS12_ggHll_pTV150_250_Nj1 (double sqrt_s) const |
| The STXS bin \(gg \to H\ell\ell\), \(N_j = 1,~150<p_{TV}[GeV]<250\). More... | |
| virtual const double | STXS12_ggHll_pTV250_Inf (double sqrt_s) const |
| The STXS bin \(gg \to H\ell\ell\), \(250 < p_{TV}[GeV]\). More... | |
| virtual const double | STXS12_ggHll_pTV75_150 (double sqrt_s) const |
| The STXS bin \(gg \to H\ell\ell\), \(75<p_{TV}[GeV]<150\). More... | |
| virtual const double | STXS12_qqHll_pTV0_75 (double sqrt_s) const |
| The STXS bin \(qq \to H\ell\ell\), \(p_{TV}[GeV]<75\). More... | |
| virtual const double | STXS12_qqHll_pTV150_250_Nj0 (double sqrt_s) const |
| The STXS bin \(qq \to H\ell\ell\), \(N_j = 0,~150<p_{TV}[GeV]<250\). More... | |
| virtual const double | STXS12_qqHll_pTV150_250_Nj1 (double sqrt_s) const |
| The STXS bin \(qq \to H\ell\ell\), \(N_j \geq 1,~150<p_{TV}[GeV]<250\). More... | |
| virtual const double | STXS12_qqHll_pTV250_Inf (double sqrt_s) const |
| The STXS bin \(qq \to H\ell\ell\), \(250<p_{TV}[GeV]\). More... | |
| virtual const double | STXS12_qqHll_pTV75_150 (double sqrt_s) const |
| The STXS bin \(qq \to H\ell\ell\), \(75<p_{TV}[GeV]<150\). More... | |
| virtual const double | STXS12_qqHlv_pTV0_75 (double sqrt_s) const |
| The STXS bin \(qq \to H\ell\nu\), \(p_{TV}[GeV]<75\). More... | |
| virtual const double | STXS12_qqHlv_pTV150_250_Nj0 (double sqrt_s) const |
| The STXS bin \(qq \to H\ell\nu\), \(N_j = 0,~150<p_{TV}[GeV]<250\). More... | |
| virtual const double | STXS12_qqHlv_pTV150_250_Nj1 (double sqrt_s) const |
| The STXS bin \(qq \to H\ell\nu\), \(N_j \geq 1,~150<p_{TV}[GeV]<250\). More... | |
| virtual const double | STXS12_qqHlv_pTV250_Inf (double sqrt_s) const |
| The STXS bin \(qq \to H\ell\nu\), \(250<p_{TV}[GeV]\). More... | |
| virtual const double | STXS12_qqHlv_pTV75_150 (double sqrt_s) const |
| The STXS bin \(qq \to H\ell\nu\), \(75<p_{TV}[GeV]<150\). More... | |
| virtual const double | STXS12_qqHqq_mjj0_60_Nj2 (double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~m_{jj}[GeV]<60\). More... | |
| virtual const double | STXS12_qqHqq_mjj120_350_Nj2 (double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~120<m_{jj}[GeV]<350\). More... | |
| virtual const double | STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj0_25_Nj2 (double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200,~p_{THjj}[GeV]<25\). More... | |
| virtual const double | STXS12_qqHqq_mjj350_700_pTH0_200_pTHjj25_Inf_Nj2 (double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200,~25<p_{THjj}[GeV]\). More... | |
| virtual const double | STXS12_qqHqq_mjj350_Inf_pTH200_Inf_Nj2 (double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV],~200<p_{TH}[GeV]\). More... | |
| virtual const double | STXS12_qqHqq_mjj60_120_Nj2 (double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~60<m_{jj}[GeV]<120\). More... | |
| virtual const double | STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj0_25_Nj2 (double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH}[GeV]<200,~p_{THjj}[GeV]<25\). More... | |
| virtual const double | STXS12_qqHqq_mjj700_Inf_pTH0_200_pTHjj25_Inf_Nj2 (double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH}[GeV]<200,~25<p_{THjj}[GeV]\). More... | |
| virtual const double | STXS12_qqHqq_Nj0 (double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j = 0\). More... | |
| virtual const double | STXS12_qqHqq_Nj1 (double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j = 1\). More... | |
| virtual const double | STXS12_tH (double sqrt_s) const |
| The STXS bin \(pp \to tH\). More... | |
| virtual const double | STXS12_ttH_pTH0_60 (double sqrt_s) const |
| The STXS bin \(pp \to ttH\), \(p_{TH}[GeV]<60\). More... | |
| virtual const double | STXS12_ttH_pTH120_200 (double sqrt_s) const |
| The STXS bin \(pp \to ttH\), \(120<p_{TH}[GeV]<200\). More... | |
| virtual const double | STXS12_ttH_pTH200_300 (double sqrt_s) const |
| The STXS bin \(pp \to ttH\), \(200<p_{TH}[GeV]<300\). More... | |
| virtual const double | STXS12_ttH_pTH300_Inf (double sqrt_s) const |
| The STXS bin \(pp \to ttH\), \(300<p_{TH}[GeV]\). More... | |
| virtual const double | STXS12_ttH_pTH60_120 (double sqrt_s) const |
| The STXS bin \(pp \to ttH\), \(60<p_{TH}[GeV]<120\). More... | |
| virtual const double | STXS_ggH0j (double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH1j_pTH_0_60 (double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH1j_pTH_120_200 (double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH1j_pTH_200 (double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH1j_pTH_60_120 (double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH2j_pTH_0_200 (double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH2j_pTH_0_60 (double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH2j_pTH_120_200 (double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH2j_pTH_200 (double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH2j_pTH_60_120 (double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH_VBFtopo_j3 (double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_ggH_VBFtopo_j3v (double sqrt_s) const |
| The STXS bin \(gg \to H\). More... | |
| virtual const double | STXS_qqHll_pTV_0_150 (double sqrt_s) const |
| The STXS bin \(qq \to H \ell \ell\). More... | |
| virtual const double | STXS_qqHll_pTV_150_250 (double sqrt_s) const |
| The STXS bin \(qq \to H \ell \ell\). More... | |
| virtual const double | STXS_qqHll_pTV_150_250_0j (double sqrt_s) const |
| The STXS bin \(qq \to H \ell \ell\). More... | |
| virtual const double | STXS_qqHll_pTV_150_250_1j (double sqrt_s) const |
| The STXS bin \(qq \to H \ell \ell\). More... | |
| virtual const double | STXS_qqHll_pTV_250 (double sqrt_s) const |
| The STXS bin \(qq \to H \ell \ell\). More... | |
| virtual const double | STXS_qqHlv_pTV_0_150 (double sqrt_s) const |
| The STXS bin \(qq \to H \ell \nu\). More... | |
| virtual const double | STXS_qqHlv_pTV_0_250 (double sqrt_s) const |
| The STXS bin \(qq \to H \ell \nu\). More... | |
| virtual const double | STXS_qqHlv_pTV_150_250_0j (double sqrt_s) const |
| The STXS bin \(qq \to H \ell \nu\). More... | |
| virtual const double | STXS_qqHlv_pTV_150_250_1j (double sqrt_s) const |
| The STXS bin \(qq \to H \ell \nu\). More... | |
| virtual const double | STXS_qqHlv_pTV_250 (double sqrt_s) const |
| The STXS bin \(qq \to H \ell \nu\). More... | |
| virtual const double | STXS_qqHqq_nonVHtopo (double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual const double | STXS_qqHqq_pTj_200 (double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual const double | STXS_qqHqq_Rest (double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual const double | STXS_qqHqq_VBFtopo_j3 (double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual const double | STXS_qqHqq_VBFtopo_j3v (double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual const double | STXS_qqHqq_VBFtopo_Rest (double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual const double | STXS_qqHqq_VHtopo (double sqrt_s) const |
| The STXS bin \(qq \to H qq\). More... | |
| virtual const double | STXS_ttHtH (double sqrt_s) const |
| The STXS bin \( ttH + tH \). More... | |
| virtual const double | STXS_WHqqHqq_pTj1_200 (double sqrt_s) const |
| The STXS bin \( qq \to WH \to H qq \). More... | |
| virtual const double | STXS_WHqqHqq_Rest (double sqrt_s) const |
| The STXS bin \( qq \to WH \to H qq \). More... | |
| virtual const double | STXS_WHqqHqq_VBFtopo_j3 (double sqrt_s) const |
| The STXS bin \( qq \to WH \to H qq \). More... | |
| virtual const double | STXS_WHqqHqq_VBFtopo_j3v (double sqrt_s) const |
| The STXS bin \( qq \to WH \to H qq \). More... | |
| virtual const double | STXS_WHqqHqq_VH2j (double sqrt_s) const |
| The STXS bin \( qq \to WH \to H qq \). More... | |
| virtual const double | STXS_ZHqqHqq_pTj1_200 (double sqrt_s) const |
| The STXS bin \( qq \to ZH \to H qq \). More... | |
| virtual const double | STXS_ZHqqHqq_Rest (double sqrt_s) const |
| The STXS bin \( qq \to ZH \to H qq \). More... | |
| virtual const double | STXS_ZHqqHqq_VBFtopo_j3 (double sqrt_s) const |
| The STXS bin \( qq \to ZH \to H qq \). More... | |
| virtual const double | STXS_ZHqqHqq_VBFtopo_j3v (double sqrt_s) const |
| The STXS bin \( qq \to ZH \to H qq \). More... | |
| virtual const double | STXS_ZHqqHqq_VH2j (double sqrt_s) const |
| The STXS bin \( qq \to ZH \to H qq \). More... | |
| const double | tovers2 (const double cosmin, const double cosmax) const |
| const double | uovers2 (const double cosmin, const double cosmax) const |
| virtual const double | xseeWW (double sqrt_s) const |
| Total \(e^+ e^- \to W^+ W^- \to jj \ell \nu\) cross section in pb, with \(\ell= e, \mu\). More... | |
| virtual const double | xseeWW4fLEP2 (double sqrt_s, const int fstate) const |
| The cross section in pb for \(e^+ e^- \to W^+ W^- \to 4f \), with \( 4f = 0 (jjjj), 1 (e v jj), 2 (mu v jj), 3 (tau v jj), 4 (e v e v), 5 (mu v mu v), 6 (tau v tau v), 7 (e v mu v), 8 (e v tau v), 9 (mu v tau v), 10 (l v jj), 11 (l v l v) \) the different fermion final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. More... | |
| virtual const double | xseeWWtotLEP2 (double sqrt_s) const |
| The total cross section in pb for \(e^+ e^- \to W^+ W^-\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. More... | |
| Public Member Functions inherited from NPbase | |
| virtual const double | A_f (const Particle f) const |
| The left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\mathcal{A}_f\). More... | |
| virtual const double | AFB (const Particle f) const |
| The forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(A^f_{FB}\). More... | |
| virtual const double | alrmoller (const double q2, const double y) const |
| virtual const double | amuon () const |
| virtual const double | BR_Zf (const Particle f) const |
| The Branching ratio of the \(Z\) boson into a given fermion pair, \(BR_Z^{f}\). More... | |
| virtual const double | BrHlljjRatio () const |
| The ratio of the Br \((H\to l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. More... | |
| virtual const double | BrHssRatio () const |
| The ratio of the Br \((H\to s\bar{s})\) in the current model and in the Standard Model. More... | |
| virtual const double | C1eeHvv (const double sqrt_s) const |
| The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More... | |
| virtual const double | C1eettH (const double sqrt_s) const |
| The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More... | |
| virtual const double | C1eeWBF (const double sqrt_s) const |
| The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More... | |
| virtual const double | C1eeZBF (const double sqrt_s) const |
| The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More... | |
| virtual const double | C1eeZH (const double sqrt_s) const |
| The C1 value controlling linear corrections from the Higgs self-coupling to single-Higgs processes for ZH. More... | |
| const double | C1Htot () const |
| The C1 coefficient controlling the H^3 corrections to the total Higgs width from the Higgs trilinear coupling. More... | |
| virtual const double | cbminuscc () const |
| virtual const double | cbminusctau () const |
| virtual const double | cbW_TWG (const double mu) const |
| virtual const double | ccminusctau () const |
| virtual const double | cgaplusct () const |
| virtual const double | cgminuscga () const |
| virtual const double | cgplusct () const |
| virtual const double | cHb_TWG (const double mu) const |
| virtual const double | cHQ3_TWG (const double mu) const |
| virtual const double | cHQm_TWG (const double mu) const |
| virtual const double | cHQp_TWG (const double mu) const |
| virtual const double | cHt_TWG (const double mu) const |
| virtual const double | cHtb_TWG (const double mu) const |
| virtual const double | cQd1_TWG (const double mu) const |
| virtual const double | cQd8_TWG (const double mu) const |
| virtual const double | cQe_TWG (const double mu) const |
| virtual const double | cQl3_TWG (const double mu) const |
| virtual const double | cQlM_TWG (const double mu) const |
| virtual const double | cQlP_TWG (const double mu) const |
| virtual const double | cQq11_TWG (const double mu) const |
| virtual const double | cQq18_TWG (const double mu) const |
| virtual const double | cQQ1_TWG (const double mu) const |
| virtual const double | cQq31_TWG (const double mu) const |
| virtual const double | cQq38_TWG (const double mu) const |
| virtual const double | cQQ8_TWG (const double mu) const |
| virtual const double | cQt1_TWG (const double mu) const |
| virtual const double | cQt8_TWG (const double mu) const |
| virtual const double | cQu1_TWG (const double mu) const |
| virtual const double | cQu8_TWG (const double mu) const |
| virtual const double | ctd1_TWG (const double mu) const |
| virtual const double | ctd8_TWG (const double mu) const |
| virtual const double | cte_TWG (const double mu) const |
| virtual const double | ctG_TWG (const double mu) const |
| virtual const double | ctH_TWG (const double mu) const |
| virtual const double | ctl_TWG (const double mu) const |
| virtual const double | ctlS_TWG (const double mu) const |
| virtual const double | ctlT_TWG (const double mu) const |
| virtual const double | ctq1_TWG (const double mu) const |
| virtual const double | ctq8_TWG (const double mu) const |
| virtual const double | ctt1_TWG (const double mu) const |
| virtual const double | ctu1_TWG (const double mu) const |
| virtual const double | ctu8_TWG (const double mu) const |
| virtual const double | ctW_TWG (const double mu) const |
| virtual const double | ctZ_TWG (const double mu) const |
| virtual const double | cVpluscb () const |
| virtual const double | cVplusctau () const |
| virtual const double | delta_alrmoller (const double q2, const double y) const |
| The computation of the parity violating asymmetry in Moller scattering. More... | |
| virtual const double | delta_amuon () const |
| The computation of the anomalous magnetic moment of the muon \(a_\mu=(g_\mu-2)/2\). More... | |
| virtual const double | delta_gAnue () const |
| The computation of the correction to the effective (muon) neutrino-electron vector coupling: delta_gAnue. More... | |
| virtual const double | delta_gLnuN2 () const |
| The computation of the correction to the effective neutrino nucleon LH coupling: delta_gLnuN2. More... | |
| virtual const double | delta_gRnuN2 () const |
| The computation of the correction to the effective neutrino nucleon RH coupling: delta_gRnuN2. More... | |
| virtual const double | delta_gVnue () const |
| The computation of the correction to the effective (muon) neutrino-electron vector coupling: delta_gVnue. More... | |
| virtual const double | delta_Qwemoller (const double q2, const double y) const |
| The computation of the electron's weak charge. More... | |
| virtual const double | delta_Qwn () const |
| The computation of the neutron weak charge: Qwn. More... | |
| virtual const double | delta_Qwp () const |
| The computation of the proton weak charge: Qwp. More... | |
| virtual const double | delta_TauLFU_gmuge () const |
| The computation of the correction to the LFU ratio \(g_\mu/ g_e \). More... | |
| virtual const double | delta_TauLFU_gtauge () const |
| The computation of the correction to the LFU ratio \(g_\tau/ g_e \). More... | |
| virtual const double | delta_TauLFU_gtaugmu () const |
| The computation of the correction to the LFU ratio \(g_\tau/ g_\mu \). More... | |
| virtual const double | delta_TauLFU_gtaugmuK () const |
| The computation of the correction to the LFU ratio \(\left(g_\tau/ g_\mu\right)_K \). More... | |
| virtual const double | delta_TauLFU_gtaugmuPi () const |
| The computation of the correction to the LFU ratio \(\left(g_\tau/ g_\mu\right)_\pi \). More... | |
| virtual const double | deltaA_f (const Particle f) const |
| The new physics contribution to the left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta \mathcal{A}_f\). More... | |
| virtual const double | deltaA_f_2 (const Particle f) const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\Delta \mathcal{A}_f^{(2)}\). More... | |
| virtual const double | deltaAFB (const Particle f) const |
| The new physics contribution to the forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta A^f_{FB}\). More... | |
| virtual const double | deltaAFB_2 (const Particle f) const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics to the forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\Delta A^f_{FB}\). More... | |
| virtual const double | deltaeNP (const double mu) const |
| The new physics relative contribution to the EW coupling constant \(e\). More... | |
| virtual const double | deltaG1_hWW_mu (const double mu) const |
| The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\). More... | |
| virtual const double | deltaG1_hZA_mu (const double mu) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\). More... | |
| virtual const double | deltaG1_hZARatio_mu (const double mu) const |
| The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More... | |
| virtual const double | deltaG1_hZZ_mu (const double mu) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\). More... | |
| virtual const double | deltaG2_hWW_mu (const double mu) const |
| The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\). More... | |
| virtual const double | deltaG2_hZA_mu (const double mu) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\). More... | |
| virtual const double | deltaG2_hZZ_mu (const double mu) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\). More... | |
| virtual const double | deltaG3_hWW_mu (const double mu) const |
| The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\). More... | |
| virtual const double | deltaG3_hZZ_mu (const double mu) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\). More... | |
| virtual const double | deltaG_hAA_mu (const double mu) const |
| The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\). More... | |
| virtual const double | deltaG_hAARatio_mu (const double mu) const |
| The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More... | |
| virtual gslpp::complex | deltaG_hff_mu (const Particle p, const double mu) const |
| The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\). More... | |
| virtual const double | deltaG_hgg_mu (const double mu) const |
| The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\). More... | |
| virtual const double | deltaG_hggRatio_mu (const double mu) const |
| The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More... | |
| virtual const double | deltaG_hhhRatio_mu (const double mu) const |
| The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value. More... | |
| virtual const double | deltaGamma_Z () const |
| The new physics contribution to the total decay width of the \(Z\) boson, \(\delta \Gamma_Z\). More... | |
| virtual const double | deltaGamma_Z_2 () const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the total decay width of the \(Z\) boson, \(\Delta \Gamma_Z^{(2)}\). More... | |
| virtual const double | deltaGamma_Zf (const Particle f) const |
| The new physics contribution to the decay width of the \(Z\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\). More... | |
| virtual const double | deltaGamma_Zf_2 (const Particle f) const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the decay width of the \(Z\) boson into a given fermion pair, \(\Delta \Gamma_{Z,f}^{(2)}\). More... | |
| virtual const double | deltaGamma_Zhad () const |
| The new physics contribution to the hadronic decay width of the \(Z\) boson, \(\delta \Gamma_{Z,had}\). More... | |
| virtual const double | deltaGamma_Zhad_2 () const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the hadronic decay width of the \(Z\) boson, \(\Delta \Gamma_{Z,had}^{(2)}\). More... | |
| const double | deltaGL_f_mu (const Particle p, const double mu) const |
| New physics contribution to the neutral-current left-handed coupling \(g_L^f\). More... | |
| virtual gslpp::complex | deltaGL_Wff_mu (const Particle pbar, const Particle p, const double mu) const |
| New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\). More... | |
| const double | deltaGR_f_mu (const Particle p, const double mu) const |
| New physics contribution to the neutral-current right-handed coupling \(g_R^f\). More... | |
| virtual gslpp::complex | deltaGR_Wff_mu (const Particle pbar, const Particle p, const double mu) const |
| New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\). More... | |
| virtual const double | deltaN_nu () const |
| The new physics contribution to the number of neutrinos dervied from the \(Z\) pole measurements. More... | |
| virtual const double | deltaR0_f (const Particle f) const |
| The new physics contribution to the ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos, respectively. More... | |
| virtual const double | deltaR0_f_2 (const Particle f) const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos: More... | |
| virtual const double | deltaR_inv () const |
| The new physics contribution to the ratio of invisible and leptonic (electron) decay widths of the \(Z\) boson, \(\delta R_{inv}\). More... | |
| virtual const double | deltaRuc () const |
| The new physics contribution to the ratio of the \(Z\to u\bar{u} + Z\to c\bar{c}\) width to the \(Z\)-boson hadronic width: More... | |
| virtual const double | deltaRuc_2 () const |
| The \(\mathcal{O}(1/\Lambda^4)\) new physics contribution to the ratio of the \(Z\to u\bar{u} + Z\to c\bar{c}\) width to the \(Z\)-boson hadronic width: More... | |
| virtual const double | deltaSigmaHadron () const |
| The new physics contribution to the cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\delta \sigma_h^0\). More... | |
| virtual const double | deltaSigmaHadron_2 () const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\Delta \sigma_h^{0,(2)}\). More... | |
| virtual const double | deltaSin2thetaEff_e () const |
| The new physics contribution to the effective electron/leptonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\rm lept}\) at the \(Z\) pole. More... | |
| virtual const double | deltaSin2thetaEff_e_2 () const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the effective electron weak angle \(\Delta \sin^2\theta_{eff,e}^{(2)}\) at the \(Z\) pole. More... | |
| virtual const double | deltaSin2thetaEff_mu () const |
| The new physics contribution to the effective muonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\mu\mu}\) at the \(Z\) pole. More... | |
| virtual const double | deltaSin2thetaEff_mu_2 () const |
| The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the effective muonic weak angle \(\Delta \sin^2\theta_{eff, \mu}^{(2)}\) at the \(Z\) pole. More... | |
| virtual const double | deltaxseeWWhadLEP2 (const double sqrt_s) const |
| The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to j j j j\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More... | |
| virtual const double | deltaxseeWWleptLEP2 (const double sqrt_s) const |
| The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to \ell \nu \ell \nu\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More... | |
| virtual const double | deltaxseeWWsemilLEP2 (const double sqrt_s) const |
| The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to \ell \nu j j\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More... | |
| virtual const double | eeffAFBbottom (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffAFBcharm (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffAFBe (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffAFBetsub (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffAFBmu (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffAFBstrange (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffAFBtau (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffRbottom (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffRcharm (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffRelectron (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffRelectrontsub (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffRmuon (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffRstrange (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffRtau (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffsigmaBottom (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffsigmaCharm (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffsigmaE (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffsigmaEtsub (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffsigmaHadron (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffsigmaMu (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffsigmaStrange (const double pol_e, const double pol_p, const double s) const |
| virtual const double | eeffsigmaTau (const double pol_e, const double pol_p, const double s) const |
| virtual const gslpp::complex | gA_f (const Particle f) const |
| The total (SM+NP) contribution to the neutral-current axial-vector coupling \(g_A^f\). More... | |
| virtual const double | Gamma_had () const |
| The hadronic decay width of the \(Z\) boson, \(\Gamma_{Z,had}\). More... | |
| virtual const double | Gamma_Z () const |
| The total decay width of the \(Z\) boson, \(\Gamma_Z\). More... | |
| virtual const double | Gamma_Zf (const Particle f) const |
| The decay width of the \(Z\) boson into a given fermion pair, \(\Gamma_Z^{f}\). More... | |
| virtual const double | GammaHssRatio () const |
| The ratio of the \(\Gamma(H\to s\bar{s})\) in the current model and in the Standard Model. More... | |
| virtual const double | gAnue () const |
| virtual const StandardModel & | getTrueSM () const |
| A method to return a StandardModel object from NPbase. More... | |
| virtual const double | gLnuN2 () const |
| virtual const double | gRnuN2 () const |
| virtual const gslpp::complex | gV_f (const Particle f) const |
| The total (SM+NP) contribution to the neutral-current vector coupling \(g_V^f\). More... | |
| virtual const double | gVnue () const |
| virtual const double | IctW_TWG (const double mu) const |
| virtual const double | IctZ_TWG (const double mu) const |
| virtual const double | kappaW4feff () const |
| The effective coupling \(\kappa_{W4f,eff}=\sqrt{\Gamma_{H4f, CC}/\Gamma_{H4f, CC}^{SM}}\). More... | |
| virtual const double | kappaZ4feff () const |
| The effective coupling \(\kappa_{Z4f,eff}=\sqrt{\Gamma_{H4f, NC}/\Gamma_{H4f, NC}^{SM}}\). More... | |
| virtual const gslpp::complex | kappaZ_f (const Particle f) const |
| The effective neutral-current coupling \(\kappa_Z^f\) including SM plus NP contributions. More... | |
| virtual const double | LEP2AFBbottom (const double s) const |
| virtual const double | LEP2AFBcharm (const double s) const |
| virtual const double | LEP2AFBe (const double s) const |
| virtual const double | LEP2AFBmu (const double s) const |
| virtual const double | LEP2AFBtau (const double s) const |
| virtual const double | LEP2dsigmadcosBinE (const double s, const double cos, const double cosmin, const double cosmax) const |
| virtual const double | LEP2dsigmadcosBinMu (const double s, const double cos, const double cosmin, const double cosmax) const |
| virtual const double | LEP2dsigmadcosBinTau (const double s, const double cos, const double cosmin, const double cosmax) const |
| virtual const double | LEP2dsigmadcosE (const double s, const double cos) const |
| virtual const double | LEP2dsigmadcosMu (const double s, const double cos) const |
| virtual const double | LEP2dsigmadcosTau (const double s, const double cos) const |
| virtual const double | LEP2Rbottom (const double s) const |
| virtual const double | LEP2Rcharm (const double s) const |
| virtual const double | LEP2sigmaBottom (const double s) const |
| virtual const double | LEP2sigmaCharm (const double s) const |
| virtual const double | LEP2sigmaE (const double s) const |
| virtual const double | LEP2sigmaHadron (const double s) const |
| virtual const double | LEP2sigmaMu (const double s) const |
| virtual const double | LEP2sigmaTau (const double s) const |
| virtual const double | mubbH (const double sqrt_s) const |
| The ratio \(\mu_{bbH}\) between the bbH production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueeHee (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{e^+e^- \to He^+e^-}\) between the \( e^+e^- \to H e^+e^- \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mueeZHGen (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeZH}\) between the \( e^{+}e^{-}\to ZH \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | muggHgagaInt (const double sqrt_s) const |
| The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. Includes interference effects with the background, following arXiv:1704.08259. More... | |
| virtual const double | muggHpbbH_Hgaga (const double sqrt_s) const |
| virtual const double | muggHpbbH_Htautau (const double sqrt_s) const |
| virtual const double | muggHpbbH_HWW (const double sqrt_s) const |
| virtual const double | muggHpbbH_HZZ (const double sqrt_s) const |
| virtual const double | muggHpttHptHpbbH_Hmumu (const double sqrt_s) const |
| virtual const double | muggHpttHptHpbbH_HZga (const double sqrt_s) const |
| virtual const double | muggHpVBFpbbH_Hbb (const double sqrt_s) const |
| virtual const double | muppHmumu (const double sqrt_s) const |
| virtual const double | muppHZga (const double sqrt_s) const |
| virtual const double | mutH (const double sqrt_s) const |
| The ratio \(\mu_{tH}\) between the t-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual const double | mutHgaga (const double sqrt_s) const |
| virtual const double | muttHptH_Hbb (const double sqrt_s) const |
| virtual const double | muttHptH_Hgaga (const double sqrt_s) const |
| virtual const double | muttHptH_Hmumu (const double sqrt_s) const |
| virtual const double | muttHptH_Htautau (const double sqrt_s) const |
| virtual const double | muttHptH_HWW (const double sqrt_s) const |
| virtual const double | muttHptH_HZZ (const double sqrt_s) const |
| virtual const double | muVBFpVH_Hmumu (const double sqrt_s) const |
| virtual const double | muVBFpVH_HZga (const double sqrt_s) const |
| virtual const double | muVHcc (const double sqrt_s) const |
| virtual const double | N_nu () const |
| The number of neutrinos dervied from the \(Z\) pole measurements, \(N_{\nu}\). More... | |
| NPbase () | |
| The default constructor. More... | |
| virtual const double | Qwemoller (const double q2, const double y) const |
| virtual const double | Qwn () const |
| virtual const double | Qwp () const |
| virtual const double | R0_f (const Particle f) const |
| The ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\), \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\) and \(R_\nu^0=\Gamma_\nu/\Gamma_{\mathrm{had}}\), for charged leptons, quarks and neutrinos, respectively. More... | |
| virtual const double | R_inv () const |
| The ratio of the invisible and leptonic (electron) decay widths of the \(Z\) boson, \(R_{inv}\). More... | |
| virtual const gslpp::complex | rhoZ_f (const Particle f) const |
| The effective neutral-current coupling \(\rho_Z^f\) including SM plus NP contributions. More... | |
| virtual const double | Ruc () const |
| The ratio of the \(Z\to u\bar{u} + Z\to c\bar{c}\) width to the \(Z\)-boson hadronic width. More... | |
| virtual const double | sigma0_had () const |
| The cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\sigma_h^0\). More... | |
| virtual const double | sin2thetaEff (const Particle f) const |
| The leptonic effective weak mixing angle \(\sin^2\theta_{\rm eff}^{\rm lept}\) at the the \(Z\) pole. More... | |
| virtual const double | STXS12_ggH_mjj0_350_pTH0_60_Nj1 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 1,~m_{jj}[GeV]<350,~p_{TH} [GeV]<60\). More... | |
| virtual const double | STXS12_ggH_mjj350_700_pTH0_200_Nj2 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH} [GeV]<200\). More... | |
| virtual const double | STXS12_ggH_mjj700_Inf_pTH0_200_Nj2 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200\). More... | |
| virtual const double | STXS12_ggH_pTH10_200_Nj0 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(N_j = 0, 10<~p_{TH} [GeV]<200\). More... | |
| virtual const double | STXS12_ggH_pTH200_300 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(~200<p_{TH} [GeV]<300\). More... | |
| virtual const double | STXS12_ggH_pTH300_450 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(~300<p_{TH} [GeV]<450\). More... | |
| virtual const double | STXS12_ggH_pTH450_650 (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(450<~p_{TH} [GeV]<650\). More... | |
| virtual const double | STXS12_ggH_pTH450_Inf (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(~p_{TH} [GeV]>450\). More... | |
| virtual const double | STXS12_ggH_pTH650_Inf (const double sqrt_s) const |
| The STXS bin \(gg \to H\), \(~p_{TH} [GeV]>650\). More... | |
| virtual const double | STXS12_qqHll_pTV0_150 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\ell\), \(0<p_{TV}<150[GeV]\). More... | |
| virtual const double | STXS12_qqHll_pTV250_400 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\ell\), \(250<p_{TV}<400[GeV]\). More... | |
| virtual const double | STXS12_qqHll_pTV400_Inf (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\ell\), \(400<p_{TV}[GeV]\). More... | |
| virtual const double | STXS12_qqHlv_pTV0_150 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\nu\), \(0<p_{TV}<150[GeV]\). More... | |
| virtual const double | STXS12_qqHlv_pTV250_400 (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\nu\), \(250<p_{TV}<400[GeV]\). More... | |
| virtual const double | STXS12_qqHlv_pTV400_Inf (const double sqrt_s) const |
| The STXS bin \(qq \to H\ell\nu\), \(400<p_{TV}[GeV]\). More... | |
| virtual const double | STXS12_qqHqq_mjj1000_1500_pTH0_200_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~1000<m_{jj}[GeV]<1500,~p_{TH}[GeV]<200\). More... | |
| virtual const double | STXS12_qqHqq_mjj1000_Inf_pTH200_Inf_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~1000<m_{jj}[GeV],~p_{TH}[GeV]>200\). More... | |
| virtual const double | STXS12_qqHqq_mjj1500_Inf_pTH0_200_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~1500<m_{jj}[GeV],~p_{TH}[GeV]<200\). More... | |
| virtual const double | STXS12_qqHqq_mjj350_1000_pTH200_Inf_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<1000,~p_{TH}[GeV]>200\). More... | |
| virtual const double | STXS12_qqHqq_mjj350_700_pTH0_200_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200\). More... | |
| virtual const double | STXS12_qqHqq_mjj700_1000_pTH0_200_Nj2 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~700<m_{jj}[GeV]<1000,~p_{TH}[GeV]<200\). More... | |
| virtual const double | STXS12_qqHqq_VH_veto_Nj01 (const double sqrt_s) const |
| The STXS bin \(qq \to Hqq\), \(N_j = 0,1\) VH-veto Ref. 2402.05742. More... | |
| virtual const double | STXS12_ttH_pTH300_450 (const double sqrt_s) const |
| The STXS bin \(pp \to ttH\), \(300<p_{TH}[GeV]<450\). More... | |
| virtual const double | STXS12_ttH_pTH450_Inf (const double sqrt_s) const |
| The STXS bin \(pp \to ttH\), \(450<p_{TH}[GeV]\). More... | |
| virtual const double | TauLFU_gmuge () const |
| virtual const double | TauLFU_gtauge () const |
| virtual const double | TauLFU_gtaugmu () const |
| virtual const double | TauLFU_gtaugmuK () const |
| virtual const double | TauLFU_gtaugmuPi () const |
| virtual bool | Update (const std::map< std::string, double > &DPars) |
| The update method for NPbase. More... | |
| virtual const double | UpperLimitZgammaA (const double sqrt_s) const |
| virtual const double | UpperLimitZgammaA13 (const double sqrt_s) const |
| virtual const double | UpperLimitZgammaC (const double sqrt_s) const |
| virtual const double | UpperLimitZgammaC13 (const double sqrt_s) const |
| virtual const double | xseeWWhadLEP2 (const double sqrt_s) const |
| The cross section in pb for \(e^+ e^- \to W^+ W^- \to j j j j\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More... | |
| virtual const double | xseeWWleptLEP2 (const double sqrt_s) const |
| The cross section in pb for \(e^+ e^- \to W^+ W^- \to \ell \nu \ell \nu\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More... | |
| virtual const double | xseeWWsemilLEP2 (const double sqrt_s) const |
| The cross section in pb for \(e^+ e^- \to W^+ W^- \to \ell \nu j j\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph]. Defined only for the NPSMEFTd6 class. More... | |
| Public Member Functions inherited from StandardModel | |
| gslpp::complex | AH_f (const double tau) const |
| Fermionic loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings. More... | |
| gslpp::complex | AH_W (const double tau) const |
| W loop function entering in the calculation of the effective \(H\gamma\gamma\) coupling. More... | |
| gslpp::complex | AHZga_f (const double tau, const double lambda) const |
| Fermionic loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| gslpp::complex | AHZga_W (const double tau, const double lambda) const |
| W loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| const double | Ale (double mu, orders order, bool Nf_thr=true) const |
| The running electromagnetic coupling \(\alpha_e(\mu)\) in the \(\overline{MS}\) scheme. More... | |
| const double | ale_OS (const double mu, orders order=FULLNLO) const |
| The running electromagnetic coupling \(\alpha(\mu)\) in the on-shell scheme. More... | |
| const double | Als (const double mu, const int Nf_in, const orders order=FULLNLO) const |
| Computes the running strong coupling \(\alpha_s(\mu)\) with \(N_f\) active flavours in the \(\overline{\mathrm{MS}}\) scheme. In the cases of LO, NLO and FULLNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda(). More... | |
| const double | Als (const double mu, const orders order, const bool Nf_thr, const bool qed_flag) const |
| The running QCD coupling \(\alpha(\mu)\) in the \(\overline{MS}\) scheme including QED corrections. More... | |
| const double | Als (const double mu, const orders order=FULLNLO, const bool Nf_thr=true) const |
| const double | Alstilde5 (const double mu) const |
| The value of \(\frac{\alpha_s^{\mathrm{FULLNLO}}}{4\pi}\) at any scale \(\mu\) with the number of flavours \(n_f = 4\) and full EW corrections. More... | |
| const double | Beta_e (int nm, unsigned int nf) const |
| QED beta function coefficients - eq. (36) hep-ph/0512066. More... | |
| const double | Beta_s (int nm, unsigned int nf) const |
| QCD beta function coefficients including QED corrections - eq. (36) hep-ph/0512066. More... | |
| virtual const double | BrHtobb () const |
| The Br \((H\to b \bar{b})\) in the Standard Model. More... | |
| virtual const double | BrHtocc () const |
| The Br \((H\to c \bar{c})\) in the Standard Model. More... | |
| virtual const double | BrHtogaga () const |
| The Br \((H\to \gamma \gamma)\) in the Standard Model. More... | |
| virtual const double | BrHtogg () const |
| The Br \(\(H\to gg)\) in the Standard Model. More... | |
| virtual const double | BrHtomumu () const |
| The Br \((H\to \mu^+ \mu^-)\) in the Standard Model. More... | |
| virtual const double | BrHtoss () const |
| The Br \((H\to s \bar{s})\) in the Standard Model. More... | |
| virtual const double | BrHtotautau () const |
| The Br \((H\to \tau^+ \tau^-)\) in the Standard Model. More... | |
| virtual const double | BrHtoWWstar () const |
| The Br \((H\to W W^*)\) in the Standard Model. More... | |
| virtual const double | BrHtoZga () const |
| The Br \((H\to Z \gamma)\) in the Standard Model. More... | |
| virtual const double | BrHtoZZstar () const |
| The Br \((H\to Z Z^*)\) in the Standard Model. More... | |
| const double | c02 () const |
| The square of the cosine of the weak mixing angle \(c_0^2\) defined without weak radiative corrections. More... | |
| virtual bool | CheckFlags () const |
| A method to check the sanity of the set of model flags. More... | |
| bool | checkSMparamsForEWPO () |
| A method to check whether the parameters relevant to the EWPO are updated. More... | |
| const double | computeBrHto4f () const |
| The Br \((H\to 4f)\) in the Standard Model. More... | |
| const double | computeBrHto4l2 () const |
| The Br \((H\to 4l)\) \(l=e,\mu\) in the Standard Model. More... | |
| const double | computeBrHto4l3 () const |
| The Br \((H\to 4l)\) \(l=e,\mu,\tau\) in the Standard Model. More... | |
| const double | computeBrHto4q () const |
| The Br \((H\to 4q)\) in the Standard Model. More... | |
| const double | computeBrHto4v () const |
| The Br \((H\to 4\nu)\) in the Standard Model. More... | |
| const double | computeBrHtobb () const |
| The Br \((H\to bb)\) in the Standard Model. More... | |
| const double | computeBrHtocc () const |
| The Br \((H\to cc)\) in the Standard Model. More... | |
| const double | computeBrHtoevmuv () const |
| The Br \((H\to e \nu \mu \nu)\) in the Standard Model. More... | |
| const double | computeBrHtogaga () const |
| The Br \((H\to\gamma\gamma)\) in the Standard Model. More... | |
| const double | computeBrHtogg () const |
| The Br \((H\to gg)\) in the Standard Model. More... | |
| const double | computeBrHtollvv2 () const |
| The Br \((H\to l^+ l^- \nu \nu)\) \(l=e,\mu\) in the Standard Model. More... | |
| const double | computeBrHtollvv3 () const |
| The Br \((H\to l^+ l^- \nu \nu)\) \(l=e,\mu,\tau\) in the Standard Model. More... | |
| const double | computeBrHtomumu () const |
| The Br \((H\to \mu\mu)\) in the Standard Model. More... | |
| const double | computeBrHtoss () const |
| The Br \((H\to ss)\) in the Standard Model. More... | |
| const double | computeBrHtotautau () const |
| The Br \((H\to \tau\tau)\) in the Standard Model. More... | |
| const double | computeBrHtoWW () const |
| The Br \((H\to WW)\) in the Standard Model. More... | |
| const double | computeBrHtoZga () const |
| The Br \((H\to Z\gamma)\) in the Standard Model. More... | |
| const double | computeBrHtoZZ () const |
| The Br \((H\to ZZ)\) in the Standard Model. More... | |
| void | ComputeDeltaR_rem (const double Mw_i, double DeltaR_rem[orders_EW_size]) const |
| A method to collect \(\Delta r_{\mathrm{rem}}\) computed via subclasses. More... | |
| void | ComputeDeltaRho (const double Mw_i, double DeltaRho[orders_EW_size]) const |
| A method to collect \(\Delta\rho\) computed via subclasses. More... | |
| const double | computeGammaHgaga_tt () const |
| The top loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More... | |
| const double | computeGammaHgaga_tW () const |
| The mixed \(t-W\) loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More... | |
| const double | computeGammaHgaga_WW () const |
| The \(W\) loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More... | |
| const double | computeGammaHgg_bb () const |
| The bottom loop contribution to \(H\to gg\) in the Standard Model. More... | |
| const double | computeGammaHgg_tb () const |
| The top-bottom interference contribution to \(H\to gg\) in the Standard Model. More... | |
| const double | computeGammaHgg_tt () const |
| The top loop contribution to \(H\to gg\) in the Standard Model. More... | |
| const double | computeGammaHTotal () const |
| The Higgs total width in the Standard Model. More... | |
| const double | computeGammaHZga_tt () const |
| The top loop contribution to \(H\to Z\gamma\) in the Standard Model. More... | |
| const double | computeGammaHZga_tW () const |
| The mixed \(t-W\) loop contribution to \(H\to Z\gamma\) in the Standard Model. More... | |
| const double | computeGammaHZga_WW () const |
| The \(W\) loop contribution to \(H\to Z\gamma\) in the Standard Model. Currently it returns the value of tab 41 in ref. [Heinemeyer:2013tqa]. More... | |
| const double | computeSigmabbH (const double sqrt_s) const |
| The bbH production cross section in the Standard Model. More... | |
| const double | computeSigmaggH (const double sqrt_s) const |
| The ggH cross section in the Standard Model. More... | |
| const double | computeSigmaggH_bb (const double sqrt_s) const |
| The square of the bottom-quark contribution to the ggH cross section in the Standard Model. More... | |
| const double | computeSigmaggH_tb (const double sqrt_s) const |
| The top-bottom interference contribution to the ggH cross section in the Standard Model. More... | |
| const double | computeSigmaggH_tt (const double sqrt_s) const |
| The square of the top-quark contribution to the ggH cross section in the Standard Model. More... | |
| const double | computeSigmatHq (const double sqrt_s) const |
| The tHq production cross section in the Standard Model. More... | |
| const double | computeSigmattH (const double sqrt_s) const |
| The ttH production cross section in the Standard Model. More... | |
| const double | computeSigmaVBF (const double sqrt_s) const |
| The VBF cross section in the Standard Model. More... | |
| const double | computeSigmaWF (const double sqrt_s) const |
| The W fusion contribution \(\sigma_{WF}\) to higgs-production cross section in the Standard Model. More... | |
| const double | computeSigmaWH (const double sqrt_s) const |
| The WH production cross section in the Standard Model. More... | |
| const double | computeSigmaZF (const double sqrt_s) const |
| The Z fusion contribution \(\sigma_{ZF}\) to higgs-production cross section in the Standard Model. More... | |
| const double | computeSigmaZH (const double sqrt_s) const |
| The ZH production cross section in the Standard Model. More... | |
| const double | computeSigmaZWF (const double sqrt_s) const |
| The Z W interference fusion contribution \(\sigma_{ZWF}\) to higgs-production cross section in the Standard Model. More... | |
| virtual const double | cW2 () const |
| virtual const double | cW2 (const double Mw_i) const |
| The square of the cosine of the weak mixing angle in the on-shell scheme, denoted as \(c_W^2\). More... | |
| virtual const double | Dalpha5hMz () const |
| The 5-quark contribution to the running of the em constant to the \(Z\) pole. \(\Delta\alpha_{had}^{(5)}(M_Z)\). More... | |
| const double | DeltaAlpha () const |
| The total corrections to the electromagnetic coupling \(\alpha\) at the \(Z\)-mass scale, denoted as \(\Delta\alpha(M_Z^2)\). More... | |
| const double | DeltaAlphaL5q () const |
| The sum of the leptonic and the five-flavour hadronic corrections to the electromagnetic coupling \(\alpha\) at the \(Z\)-mass scale, denoted as \(\Delta\alpha^{\ell+5q}(M_Z^2)\). More... | |
| const double | DeltaAlphaLepton (const double s) const |
| Leptonic contribution to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{lept}}(s)\). More... | |
| const double | DeltaAlphaTop (const double s) const |
| Top-quark contribution to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{top}}(s)\). More... | |
| virtual const gslpp::complex | deltaKappaZ_f (const Particle f) const |
| Flavour non-universal vertex corrections to \(\kappa_Z^l\), denoted by \(\Delta\kappa_Z^l\). More... | |
| virtual const double | DeltaR () const |
| The SM prediction for \(\Delta r\) derived from that for the \(W\) boson mass. More... | |
| virtual const double | DeltaRbar () const |
| The SM prediction for \(\Delta \overline{r}\) derived from that for the \(W\)-boson mass. More... | |
| virtual const gslpp::complex | deltaRhoZ_f (const Particle f) const |
| Flavour non-universal vertex corrections to \(\rho_Z^l\), denoted by \(\Delta\rho_Z^l\). More... | |
| const double | eeffsigma (const Particle f, const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const |
| const double | eeffsigmaEbin (const double pol_e, const double pol_p, const double s, const double cosmin, const double cosmax) const |
| virtual const double | epsilon1 () const |
| The SM contribution to the epsilon parameter \(\varepsilon_1\). More... | |
| virtual const double | epsilon2 () const |
| The SM contribution to the epsilon parameter \(\varepsilon_2\). More... | |
| virtual const double | epsilon3 () const |
| The SM contribution to the epsilon parameter \(\varepsilon_3\). More... | |
| virtual const double | epsilonb () const |
| The SM contribution to the epsilon parameter \(\varepsilon_b\). More... | |
| gslpp::complex | f_triangle (const double tau) const |
| Loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings. More... | |
| gslpp::complex | g_triangle (const double tau) const |
| Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| virtual const double | Gamma_inv () const |
| The invisible partial decay width of the \(Z\) boson, \(\Gamma_{\mathrm{inv}}\). More... | |
| virtual const double | Gamma_muon () const |
| The computation of the muon decay. More... | |
| virtual const double | Gamma_tau_l_nunu (const Particle l) const |
| The computation of the leptonic tau decays. More... | |
| virtual const double | GammaHtobb () const |
| The \(\Gamma(H\to b \bar{b})\) in the Standard Model. More... | |
| virtual const double | GammaHtocc () const |
| The \(\Gamma(H\to c \bar{c})\) in the Standard Model. More... | |
| virtual const double | GammaHtogaga () const |
| The \(\Gamma(H\to \gamma \gamma)\) in the Standard Model. More... | |
| virtual const double | GammaHtogg () const |
| The \(\Gamma(H\to gg)\) in the Standard Model. More... | |
| virtual const double | GammaHtomumu () const |
| The \(\Gamma(H\to \mu^+ \mu^-)\) in the Standard Model. More... | |
| virtual const double | GammaHtoss () const |
| The \(\Gamma(H\to s \bar{s})\) in the Standard Model. More... | |
| virtual const double | GammaHTot () const |
| The total Higgs width \(\Gamma(H)\) in the Standard Model. More... | |
| virtual const double | GammaHtotautau () const |
| The \(\Gamma(H\to \tau^+ \tau^-)\) in the Standard Model. More... | |
| virtual const double | GammaHtoWWstar () const |
| The \(\Gamma(H\to W W^*)\) in the Standard Model. More... | |
| virtual const double | GammaHtoZga () const |
| The \(\Gamma(H\to Z \gamma)\) in the Standard Model. More... | |
| virtual const double | GammaHtoZZstar () const |
| The \(\Gamma(H\to Z Z^*)\) in the Standard Model. More... | |
| virtual const double | GammaZ (const Particle f) const |
| The \(Z\to \ell\bar{\ell}\) partial decay width, \(\Gamma_\ell\). More... | |
| const double | getAle () const |
| A get method to retrieve the fine-structure constant \(\alpha\). More... | |
| const double | getAlsMz () const |
| A get method to access the value of \(\alpha_s(M_Z)\). More... | |
| virtual const double | getCBd () const |
| The ratio of the absolute value of the $B_d$ mixing amplitude over the Standard Model value. More... | |
| virtual const double | getCBs () const |
| The ratio of the absolute value of the $B_s$ mixing amplitude over the Standard Model value. More... | |
| virtual const double | getCCC1 () const |
| A virtual implementation for the RealWeakEFTCC class. More... | |
| virtual const double | getCCC2 () const |
| A virtual implementation for the RealWeakEFTCC class. More... | |
| virtual const double | getCCC3 () const |
| A virtual implementation for the RealWeakEFTCC class. More... | |
| virtual const double | getCCC4 () const |
| A virtual implementation for the RealWeakEFTCC class. More... | |
| virtual const double | getCCC5 () const |
| A virtual implementation for the RealWeakEFTCC class. More... | |
| virtual const double | getCDMK () const |
| The ratio of the real part of the $K$ mixing amplitude over the Standard Model value. More... | |
| virtual const double | getCepsK () const |
| The ratio of the imaginary part of the $K$ mixing amplitude over the Standard Model value. More... | |
| const CKM & | getCKM () const |
| A get method to retrieve the member object of type CKM. More... | |
| const double | getDAle5Mz () const |
| A get method to retrieve the five-flavour hadronic contribution to the electromagnetic coupling, \(\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)\). More... | |
| const double | getDelGammaZ () const |
| A get method to retrieve the theoretical uncertainty in \(\Gamma_Z\), denoted as \(\delta\,\Gamma_Z\). More... | |
| const double | getDelMw () const |
| A get method to retrieve the theoretical uncertainty in \(M_W\), denoted as \(\delta\,M_W\). More... | |
| const double | getDelR0b () const |
| A get method to retrieve the theoretical uncertainty in \(R_b^0\), denoted as \(\delta\,R_b^0\). More... | |
| const double | getDelR0c () const |
| A get method to retrieve the theoretical uncertainty in \(R_c^0\), denoted as \(\delta\,R_c^0\). More... | |
| const double | getDelR0l () const |
| A get method to retrieve the theoretical uncertainty in \(R_l^0\), denoted as \(\delta\,R_l^0\). More... | |
| const double | getDelSigma0H () const |
| A get method to retrieve the theoretical uncertainty in \(\sigma_{Hadron}^0\), denoted as \(\delta\,\sigma_{Hadron}^0\). More... | |
| const double | getDelSin2th_b () const |
| A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{b}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{b}\). More... | |
| const double | getDelSin2th_l () const |
| A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{\rm lept}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{\rm lept}\). More... | |
| const double | getDelSin2th_q () const |
| A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{q\not = b,t}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{q\not = b,t}\). More... | |
| const std::string | getFlagKappaZ () const |
| A method to retrieve the model flag KappaZ. More... | |
| const std::string | getFlagMw () const |
| A method to retrieve the model flag Mw. More... | |
| const std::string | getFlagRhoZ () const |
| A method to retrieve the model flag RhoZ. More... | |
| const Flavour & | getFlavour () const |
| const double | getGF () const |
| A get method to retrieve the Fermi constant \(G_\mu\). More... | |
| const int | getIterationNo () const |
| const Particle & | getLeptons (const QCD::lepton p) const |
| A get method to retrieve the member object of a lepton. More... | |
| virtual const double | getMHl () const |
| A get method to retrieve the Higgs mass \(m_h\). More... | |
| virtual const double | getmq (const QCD::quark q, const double mu) const |
| The MSbar running quark mass computed at NLO. More... | |
| const double | getMuw () const |
| A get method to retrieve the matching scale \(\mu_W\) around the weak scale. More... | |
| const double | getMw () const |
| A get method to access the input value of the mass of the \(W\) boson \(M_W\). More... | |
| EWSMApproximateFormulae * | getMyApproximateFormulae () const |
| A get method to retrieve the member pointer of type EWSMApproximateFormulae. More... | |
| EWSMcache * | getMyEWSMcache () const |
| A get method to retrieve the member pointer of type EWSMcache. More... | |
| LeptonFlavour * | getMyLeptonFlavour () const |
| EWSMOneLoopEW * | getMyOneLoopEW () const |
| A get method to retrieve the member pointer of type EWSMOneLoopEW,. More... | |
| EWSMThreeLoopEW * | getMyThreeLoopEW () const |
| EWSMThreeLoopEW2QCD * | getMyThreeLoopEW2QCD () const |
| EWSMThreeLoopQCD * | getMyThreeLoopQCD () const |
| EWSMTwoFermionsLEP2 * | getMyTwoFermionsLEP2 () const |
| A get method to retrieve the member pointer of type EWSMTwoFermionsLEP2. More... | |
| EWSMTwoLoopEW * | getMyTwoLoopEW () const |
| EWSMTwoLoopQCD * | getMyTwoLoopQCD () const |
| const double | getMz () const |
| A get method to access the mass of the \(Z\) boson \(M_Z\). More... | |
| virtual const double | getPhiBd () const |
| Half the relative phase of the $B_d$ mixing amplitude w.r.t. the Standard Model one. More... | |
| virtual const double | getPhiBs () const |
| Half the relative phase of the $B_s$ mixing amplitude w.r.t. the Standard Model one. More... | |
| const gslpp::matrix< gslpp::complex > | getUPMNS () const |
| A get method to retrieve the object of the PMNS matrix. More... | |
| const gslpp::matrix< gslpp::complex > | getVCKM () const |
| A get method to retrieve the CKM matrix. More... | |
| const gslpp::matrix< gslpp::complex > & | getYd () const |
| A get method to retrieve the Yukawa matrix of the down-type quarks, \(Y_d\). More... | |
| const gslpp::matrix< gslpp::complex > & | getYe () const |
| A get method to retrieve the Yukawa matrix of the charged leptons, \(Y_e\). More... | |
| const gslpp::matrix< gslpp::complex > & | getYn () const |
| A get method to retrieve the Yukawa matrix of the neutrinos, \(Y_\nu\). More... | |
| const gslpp::matrix< gslpp::complex > & | getYu () const |
| A get method to retrieve the Yukawa matrix of the up-type quarks, \(Y_u\). More... | |
| gslpp::complex | I_triangle_1 (const double tau, const double lambda) const |
| Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| gslpp::complex | I_triangle_2 (const double tau, const double lambda) const |
| Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| virtual bool | Init (const std::map< std::string, double > &DPars) |
| A method to initialize the model parameters. More... | |
| virtual bool | InitializeModel () |
| A method to initialize the model. More... | |
| const double | intMLL2eeeeus2 (const double s, const double t0, const double t1) const |
| const double | intMLR2eeeets2 (const double s, const double t0, const double t1) const |
| const double | intMLRtilde2eeeest2 (const double s, const double t0, const double t1) const |
| const double | intMRR2eeeeus2 (const double s, const double t0, const double t1) const |
| const bool | IsFlagNoApproximateGammaZ () const |
| A method to retrieve the model flag NoApproximateGammaZ. More... | |
| const bool | IsFlagWithoutNonUniversalVC () const |
| A method to retrieve the model flag WithoutNonUniversalVC. More... | |
| const bool | isSMSuccess () const |
| A get method to retrieve the success status of the Standard Model update and matching. More... | |
| const double | MLL2eeff (const Particle f, const double s, const double t) const |
| const double | MLR2eeff (const Particle f, const double s) const |
| const double | MRL2eeff (const Particle f, const double s) const |
| const double | MRR2eeff (const Particle f, const double s, const double t) const |
| const double | Mw_tree () const |
| The tree-level mass of the \(W\) boson, \(M_W^{\mathrm{tree}}\). More... | |
| const double | MwbarFromMw (const double Mw) const |
| A method to convert the \(W\)-boson mass in the experimental/running-width scheme to that in the complex-pole/fixed-width scheme. More... | |
| const double | MwFromMwbar (const double Mwbar) const |
| A method to convert the \(W\)-boson mass in the complex-pole/fixed-width scheme to that in the experimental/running-width scheme. More... | |
| double | Mzbar () const |
| The \(Z\)-boson mass \(\overline{M}_Z\) in the complex-pole/fixed-width scheme. More... | |
| virtual bool | PreUpdate () |
| The pre-update method for StandardModel. More... | |
| virtual const double | rho_GammaW (const Particle fi, const Particle fj) const |
| EW radiative corrections to the width of \(W \to f_i \bar{f}_j\), denoted as \(\rho^W_{ij}\). More... | |
| const double | s02 () const |
| The square of the sine of the weak mixing angle \(s_0^2\) defined without weak radiative corrections. More... | |
| void | setCKM (const CKM &CKMMatrix) |
| A set method to change the CKM matrix. More... | |
| void | setFlagCacheInStandardModel (bool FlagCacheInStandardModel) |
| A set method to change the model flag CacheInStandardModel of StandardModel. More... | |
| void | setFlagNoApproximateGammaZ (bool FlagNoApproximateGammaZ) |
| bool | setFlagSigmaForAFB (const bool flagSigmaForAFB_i) |
| bool | setFlagSigmaForR (const bool flagSigmaForR_i) |
| virtual bool | setFlagStr (const std::string name, const std::string value) |
| A method to set a flag of StandardModel. More... | |
| void | setRequireCKM (bool requireCKM) |
| A set method to change the value of requireCKM. More... | |
| void | setSMSuccess (bool success) const |
| A set method to change the success status of the Standard Model update and matching. More... | |
| void | setYd (const gslpp::matrix< gslpp::complex > &Yd) |
| A set method to set the Yukawa matrix of the down-type quarks, \(Y_d\). More... | |
| void | setYe (const gslpp::matrix< gslpp::complex > &Ye) |
| A set method to set the Yukawa matrix of the charged leptons, \(Y_e\). More... | |
| void | setYu (const gslpp::matrix< gslpp::complex > &Yu) |
| A set method to set the Yukawa matrix of the up-type quarks, \(Y_u\). More... | |
| virtual const double | SigmaeeHee (const double sqrt_s, const double Pe, const double Pp) const |
| The \(\sigma(e^+ e^- \to e^+ e^- H)\) in the Standard Model. More... | |
| virtual const double | SigmaeeHvv (const double sqrt_s, const double Pe, const double Pp) const |
| The \(\sigma(e^+ e^- \to \nu \bar{\nu} H)\) in the Standard Model. More... | |
| virtual const double | SigmaeeZH (const double sqrt_s, const double Pe, const double Pp) const |
| The \(\sigma(e^+ e^- \to Z H)\) in the Standard Model. More... | |
| StandardModel () | |
| The default constructor. More... | |
| const double | sW2 () const |
| virtual const double | sW2 (const double Mw_i) const |
| The square of the sine of the weak mixing angle in the on-shell scheme, denoted as \(s_W^2\). More... | |
| const double | sW2_MSbar_Approx () const |
| The (approximated formula for the) square of the sine of the weak mixing angle in the MSbar scheme, denoted as \(\hat{s}_{W}^2\). See: PDG 22, R.L. Workman et al. (Particle Data Group), Prog. Theor. Exp. Phys. 2022, 083C01 (2022) More... | |
| const double | sW2_ND () const |
| The square of the sine of the weak mixing angle in the MSbar-ND scheme (w/o decoupling $\alpha\ln(m_t/M_Z)$ terms), denoted as \(\hat{s}_{ND}^2\). See: PDG 22, R.L. Workman et al. (Particle Data Group), Prog. Theor. Exp. Phys. 2022, 083C01 (2022) (eq. 10.13a/10.13b) More... | |
| virtual const double | ThetaLnuN () const |
| The effective neutrino nucleon LH parameter: ThetaLnuN. More... | |
| virtual const double | ThetaRnuN () const |
| The effective neutrino nucleon RH parameter: ThetaRnuN. More... | |
| const double | tovers2 (const double cosmin, const double cosmax) const |
| const double | uovers2 (const double cosmin, const double cosmax) const |
| const double | v () const |
| The Higgs vacuum expectation value. More... | |
| virtual | ~StandardModel () |
| The default destructor. More... | |
| Public Member Functions inherited from QCD | |
| const double | AboveTh (const double mu) const |
| The active flavour threshold above the scale \(\mu\) as defined in QCD::Thresholds(). More... | |
| void | addParameters (std::vector< std::string > params_i) |
| A method to add parameters that are specific to only one set of observables. More... | |
| const double | Als (const double mu, const int Nf_in, const orders order=FULLNLO) const |
| Computes the running strong coupling \(\alpha_s(\mu)\) with \(N_f\) active flavours in the \(\overline{\mathrm{MS}}\) scheme. In the cases of LO, NLO and FULLNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda(). More... | |
| const double | Als (const double mu, const orders order=FULLNLO, const bool Nf_thr=true) const |
| const double | Als4 (const double mu) const |
| The value of \(\alpha_s^{\mathrm{FULLNLO}}\) at any scale \(\mu\) with the number of flavours \(n_f = 4\). More... | |
| const double | AlsByOrder (const double mu, const int Nf_in, const orders order=FULLNLO) const |
| const double | AlsByOrder (const double mu, const orders order=FULLNLO, bool Nf_thr=true) const |
| const double | AlsOLD (const double mu, const orders order=FULLNLO) const |
| Computes the running strong coupling \(\alpha_s(\mu)\) in the \(\overline{\mathrm{MS}}\) scheme. In the cases of LO, NLO and FULLNNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda(). More... | |
| const double | AlsWithInit (const double mu, const double alsi, const double mu_i, const int nf, const orders order) const |
| Computes the running strong coupling \(\alpha_s(\mu)\) from \(\alpha_s(\mu_i)\) in the \(\overline{\mathrm{MS}}\) scheme, where it is forbidden to across a flavour threshold in the RG running from \(\mu_i\) to \(\mu\). More... | |
| const double | AlsWithLambda (const double mu, const orders order) const |
| Computes the running strong coupling \(\alpha_s(\mu)\) in the \(\overline{\mathrm{MS}}\) scheme with the use of \(\Lambda_{\rm QCD}\). More... | |
| const double | BelowTh (const double mu) const |
| The active flavour threshold below the scale \(\mu\) as defined in QCD::Thresholds(). More... | |
| const double | Beta0 (const double nf) const |
| The \(\beta_0(n_f)\) coefficient for a certain number of flavours \(n_f\). More... | |
| const double | Beta1 (const double nf) const |
| The \(\beta_1(n_f)\) coefficient for a certain number of flavours \(n_f\). More... | |
| const double | Beta2 (const double nf) const |
| The \(\beta_2(n_f)\) coefficient for a certain number of flavours \(n_f\). More... | |
| const double | Beta3 (const double nf) const |
| The \(\beta_3(n_f)\) coefficient for a certain number of flavours \(n_f\). More... | |
| void | CacheShift (double cache[][5], int n) const |
| A member used to manage the caching for this class. More... | |
| void | CacheShift (int cache[][5], int n) const |
| const orders | FullOrder (orders order) const |
| Return the FULLORDER enum corresponding to order. More... | |
| const double | Gamma0 (const double nf) const |
| The \(\gamma_0\) coefficient used to compute the running of a mass. More... | |
| const double | Gamma1 (const double nf) const |
| The \(\gamma_1\) coefficient used to compute the running of a mass. More... | |
| const double | Gamma2 (const double nf) const |
| The \(\gamma_2\) coefficient used to compute the running of a mass. More... | |
| const double | getAlsM () const |
| A get method to access the value of \(\alpha_s(M_{\alpha_s})\). More... | |
| const BParameter & | getBBd () const |
| For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta b = 2\) process in the \(B_d\) meson system. More... | |
| const BParameter & | getBBd_subleading () const |
| For getting the subleading bag parameters \(R_2 - R_3\) in \(\Delta b = 2\) process in the \(B_d\) meson system. More... | |
| const BParameter & | getBBs () const |
| For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta b = 2\) process in the \(B_s\) meson system. More... | |
| const BParameter & | getBBs_subleading () const |
| For getting the subleading bag parameters \(R_2 - R_3\) in \(\Delta b = 2\) process in the \(B_s\) meson system. More... | |
| const BParameter & | getBD () const |
| For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta c = 2\) process in the \(D^0\) meson system. More... | |
| const BParameter & | getBK () const |
| For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta s = 2\) process in the \(K^0\) meson system. More... | |
| const BParameter & | getBKd1 () const |
| const BParameter & | getBKd3 () const |
| const double | getCF () const |
| A get method to access the Casimir factor of QCD. More... | |
| const double | getMAls () const |
| A get method to access the mass scale \(M_{\alpha_s}\) at which the strong coupling constant measurement is provided. More... | |
| const Meson & | getMesons (const QCD::meson m) const |
| A get method to access a meson as an object of the type Meson. More... | |
| const double | getMtpole () const |
| A get method to access the pole mass of the top quark. More... | |
| const double | getMub () const |
| A get method to access the threshold between five- and four-flavour theory in GeV. More... | |
| const double | getMuc () const |
| A get method to access the threshold between four- and three-flavour theory in GeV. More... | |
| const double | getMut () const |
| A get method to access the threshold between six- and five-flavour theory in GeV. More... | |
| const double | getNc () const |
| A get method to access the number of colours \(N_c\). More... | |
| const double | getOptionalParameter (std::string name) const |
| A method to get parameters that are specific to only one set of observables. More... | |
| const Particle & | getQuarks (const QCD::quark q) const |
| A get method to access a quark as an object of the type Particle. More... | |
| std::vector< std::string > | getUnknownParameters () |
| A method to get the vector of the parameters that have been specified in the configuration file but not being used. More... | |
| void | initializeBParameter (std::string name_i) const |
| A method to initialize B Parameter and the corresponding meson. More... | |
| void | initializeMeson (QCD::meson meson_i) const |
| A method to initialize a meson. More... | |
| bool | isQCDsuccess () const |
| A getter for the QCDsuccess flag. More... | |
| const double | logLambda (const double nf, orders order) const |
| Computes \(\ln\Lambda_\mathrm{QCD}\) with nf flavours in GeV. More... | |
| const double | Mbar2Mp (const double mbar, const quark q, const orders order=FULLNNLO) const |
| Converts the \(\overline{\mathrm{MS}}\) mass \(m(m)\) to the pole mass. More... | |
| const double | Mofmu2Mbar (const double m, const double mu, const quark q) const |
| Converts a quark running mass at an arbitrary scale to the corresponding \(\overline{\mathrm{MS}}\) mass \(m(m)\). More... | |
| const double | Mp2Mbar (const double mp, const quark q, orders order=FULLNNLO) const |
| Converts a quark pole mass to the corresponding \(\overline{\mathrm{MS}}\) mass \(m(m)\). More... | |
| const double | Mrun (const double mu, const double m, const quark q, const orders order=FULLNNLO) const |
| Computes a running quark mass \(m(\mu)\) from \(m(m)\). More... | |
| const double | Mrun (const double mu_f, const double mu_i, const double m, const quark q, const orders order=FULLNNLO) const |
| Runs a quark mass from \(\mu_i\) to \(\mu_f\). More... | |
| const double | Mrun4 (const double mu_f, const double mu_i, const double m) const |
| The running of a mass with the number of flavours \(n_f = 4\). More... | |
| const double | MS2DRqmass (const double MSbar) const |
| Converts a quark mass from the \(\overline{\mathrm{MS}}\) scheme to the \(\overline{\mathrm{DR}}\) scheme. More... | |
| const double | MS2DRqmass (const double MSscale, const double MSbar) const |
| Converts a quark mass from the \(\overline{\mathrm{MS}}\) scheme to the \(\overline{\mathrm{DR}}\) scheme. More... | |
| const double | Nf (const double mu) const |
| The number of active flavour at scale \(\mu\). More... | |
| const double | NfThresholdCorrections (double mu, double M, double als, int nf, orders order) const |
| Threshold corrections in matching \(\alpha_s(n_f+1)\) with \(\alpha_s(n_f)\) from eq. (34) of hep-ph/0512060. More... | |
| const std::string | orderToString (const orders order) const |
| Converts an object of the enum type "orders" to the corresponding string. More... | |
| QCD () | |
| Constructor. More... | |
| void | setComputemt (bool computemt) |
| A set method to change the value of computemt. More... | |
| void | setMtpole (double mtpole_in) |
| A method to set the pole mass of the top quark. More... | |
| void | setNc (double Nc) |
| A set method to change the number of colours \(N_c\). More... | |
| void | setOptionalParameter (std::string name, double value) |
| A method to set the parameter value for the parameters that are specific to only one set of observables. More... | |
| void | setQuarkMass (const quark q, const double mass) |
| A set method to change the mass of a quark. More... | |
| const double | Thresholds (const int i) const |
| For accessing the active flavour threshold scales. More... | |
| Public Member Functions inherited from Model | |
| void | addMissingModelParameter (const std::string &missingParameterName) |
| std::vector< std::string > | getmissingModelParameters () |
| unsigned int | getMissingModelParametersCount () |
| std::string | getModelName () const |
| A method to fetch the name of the model. More... | |
| const double & | getModelParam (std::string name) const |
| bool | isModelFWC_DF2 () const |
| bool | isModelGeneralTHDM () const |
| bool | isModelGeorgiMachacek () const |
| bool | IsModelInitialized () const |
| A method to check if the model is initialized. More... | |
| bool | isModelLinearized () const |
| bool | isModelNPquadratic () const |
| bool | isModelParam (std::string name) const |
| bool | isModelSUSY () const |
| bool | isModelTHDM () const |
| bool | isModelTHDMW () const |
| bool | IsUpdateError () const |
| A method to check if there was any error in the model update process. More... | |
| Model () | |
| The default constructor. More... | |
| void | raiseMissingModelParameterCount () |
| void | setModelFWC_DF2 () |
| void | setModelGeneralTHDM () |
| void | setModelGeorgiMachacek () |
| void | setModelInitialized (bool ModelInitialized) |
| A set method to fix the failure or success of the initialization of the model. More... | |
| void | setModelLinearized (bool linearized=true) |
| void | setModelName (const std::string name) |
| A method to set the name of the model. More... | |
| void | setModelNPquadratic (bool NPquadratic=true) |
| void | setModelSUSY () |
| void | setModelTHDM () |
| void | setModelTHDMW () |
| void | setSliced (bool Sliced) |
| void | setUpdateError (bool UpdateError) |
| A set method to fix the update status as success or failure. More... | |
| virtual | ~Model () |
| The default destructor. More... | |
Static Public Attributes | |
| static const int | NNPSMEFTd6Vars = 557 |
| The number of the model parameters in NPSMEFTd6. More... | |
| static const int | NNPSMEFTd6Vars_LFU_QFU = 292 |
| The number of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities. More... | |
| static const std::string | NPSMEFTd6Vars [NNPSMEFTd6Vars] |
| A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotateCHWCHB=false. More... | |
| static const std::string | NPSMEFTd6Vars_LFU_QFU [NNPSMEFTd6Vars_LFU_QFU] |
| A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=false. More... | |
| static const std::string | NPSMEFTd6VarsRot [NNPSMEFTd6Vars] |
| A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotateCHWCHB=true. More... | |
| static const std::string | NPSMEFTd6VarsRot_LFU_QFU [NNPSMEFTd6Vars_LFU_QFU] |
| A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=true. More... | |
| Static Public Attributes inherited from StandardModel | |
| static const double | GeVminus2_to_nb = 389379.338 |
| static const double | Mw_error = 0.00001 |
| The target accuracy of the iterative calculation of the \(W\)-boson mass in units of GeV. More... | |
| static const int | NSMvars = 26 |
| The number of the model parameters in StandardModel. More... | |
| static const int | NumSMParamsForEWPO = 33 |
| The number of the SM parameters that are relevant to the EW precision observables. More... | |
| static std::string | SMvars [NSMvars] |
| A string array containing the labels of the model parameters in StandardModel. More... | |
| Static Public Attributes inherited from QCD | |
| static const int | NQCDvars = 11 |
| The number of model parameters in QCD. More... | |
| static std::string | QCDvars [NQCDvars] |
| An array containing the labels under which all QCD parameters are stored in a vector of ModelParameter via InputParser::ReadParameters(). More... | |
Protected Member Functions | |
| gslpp::complex | CfB_diag (const Particle f) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{EB,UB,DB}\) corresponding to particle f. More... | |
| gslpp::complex | CfG_diag (const Particle f) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{UG,DG}\) corresponding to particle f. More... | |
| gslpp::complex | CfH_diag (const Particle f) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{EH,UH,DH}\) corresponding to particle f. More... | |
| gslpp::complex | CfW_diag (const Particle f) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{EW,UW,DW}\) corresponding to particle f. More... | |
| const double | CHF1_diag (const Particle F) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(1)}\) corresponding to particle F. More... | |
| const double | CHF3_diag (const Particle F) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(3)}\) corresponding to particle F. More... | |
| const double | CHf_diag (const Particle f) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{HE,HU,HD}\) corresponding to particle f. More... | |
| gslpp::complex | CHud_diag (const Particle u) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{Hud}\) corresponding to particle f. More... | |
| virtual void | setParameter (const std::string name, const double &value) |
| A method to set the value of a parameter of the model. More... | |
| Protected Member Functions inherited from StandardModel | |
| const double | AFB_NoISR_l (const QCD::lepton l_flavor, const double s) const |
| const double | AFB_NoISR_q (const QCD::quark q_flavor, const double s) const |
| bool | checkEWPOscheme (const std::string scheme) const |
| A method to check if a given scheme name in string form is valid. More... | |
| virtual void | computeCKM () |
| The method to compute the CKM matrix. More... | |
| virtual void | computeYukawas () |
| The method to compute the Yukawas matrix. More... | |
| double | Delta_EWQCD (const QCD::quark q) const |
| The non-factorizable EW-QCD corrections to the partial widths for \(Z\to q\bar{q}\), denoted as \(\Delta_{\mathrm{EW/QCD}}\). More... | |
| const double | getIntegrand_AFBnumeratorWithISR_bottom133 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom167 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom172 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom183 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom189 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom192 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom196 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom200 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom202 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom205 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_bottom207 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm133 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm167 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm172 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm183 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm189 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm192 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm196 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm200 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm202 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm205 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_charm207 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu130 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu136 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu161 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu172 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu183 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu189 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu192 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu196 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu200 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu202 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu205 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_mu207 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau130 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau136 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau161 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau172 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau183 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau189 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau192 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau196 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau200 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau202 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau205 (double x) const |
| const double | getIntegrand_AFBnumeratorWithISR_tau207 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom130 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom133 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom136 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom161 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom167 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom172 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom183 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom189 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom192 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom196 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom200 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom202 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom205 (double x) const |
| const double | getIntegrand_dsigmaBox_bottom207 (double x) const |
| const double | getIntegrand_dsigmaBox_charm130 (double x) const |
| const double | getIntegrand_dsigmaBox_charm133 (double x) const |
| const double | getIntegrand_dsigmaBox_charm136 (double x) const |
| const double | getIntegrand_dsigmaBox_charm161 (double x) const |
| const double | getIntegrand_dsigmaBox_charm167 (double x) const |
| const double | getIntegrand_dsigmaBox_charm172 (double x) const |
| const double | getIntegrand_dsigmaBox_charm183 (double x) const |
| const double | getIntegrand_dsigmaBox_charm189 (double x) const |
| const double | getIntegrand_dsigmaBox_charm192 (double x) const |
| const double | getIntegrand_dsigmaBox_charm196 (double x) const |
| const double | getIntegrand_dsigmaBox_charm200 (double x) const |
| const double | getIntegrand_dsigmaBox_charm202 (double x) const |
| const double | getIntegrand_dsigmaBox_charm205 (double x) const |
| const double | getIntegrand_dsigmaBox_charm207 (double x) const |
| const double | getIntegrand_dsigmaBox_down130 (double x) const |
| const double | getIntegrand_dsigmaBox_down133 (double x) const |
| const double | getIntegrand_dsigmaBox_down136 (double x) const |
| const double | getIntegrand_dsigmaBox_down161 (double x) const |
| const double | getIntegrand_dsigmaBox_down167 (double x) const |
| const double | getIntegrand_dsigmaBox_down172 (double x) const |
| const double | getIntegrand_dsigmaBox_down183 (double x) const |
| const double | getIntegrand_dsigmaBox_down189 (double x) const |
| const double | getIntegrand_dsigmaBox_down192 (double x) const |
| const double | getIntegrand_dsigmaBox_down196 (double x) const |
| const double | getIntegrand_dsigmaBox_down200 (double x) const |
| const double | getIntegrand_dsigmaBox_down202 (double x) const |
| const double | getIntegrand_dsigmaBox_down205 (double x) const |
| const double | getIntegrand_dsigmaBox_down207 (double x) const |
| const double | getIntegrand_dsigmaBox_mu130 (double x) const |
| const double | getIntegrand_dsigmaBox_mu133 (double x) const |
| const double | getIntegrand_dsigmaBox_mu136 (double x) const |
| const double | getIntegrand_dsigmaBox_mu161 (double x) const |
| const double | getIntegrand_dsigmaBox_mu167 (double x) const |
| const double | getIntegrand_dsigmaBox_mu172 (double x) const |
| const double | getIntegrand_dsigmaBox_mu183 (double x) const |
| const double | getIntegrand_dsigmaBox_mu189 (double x) const |
| const double | getIntegrand_dsigmaBox_mu192 (double x) const |
| const double | getIntegrand_dsigmaBox_mu196 (double x) const |
| const double | getIntegrand_dsigmaBox_mu200 (double x) const |
| const double | getIntegrand_dsigmaBox_mu202 (double x) const |
| const double | getIntegrand_dsigmaBox_mu205 (double x) const |
| const double | getIntegrand_dsigmaBox_mu207 (double x) const |
| const double | getIntegrand_dsigmaBox_strange130 (double x) const |
| const double | getIntegrand_dsigmaBox_strange133 (double x) const |
| const double | getIntegrand_dsigmaBox_strange136 (double x) const |
| const double | getIntegrand_dsigmaBox_strange161 (double x) const |
| const double | getIntegrand_dsigmaBox_strange167 (double x) const |
| const double | getIntegrand_dsigmaBox_strange172 (double x) const |
| const double | getIntegrand_dsigmaBox_strange183 (double x) const |
| const double | getIntegrand_dsigmaBox_strange189 (double x) const |
| const double | getIntegrand_dsigmaBox_strange192 (double x) const |
| const double | getIntegrand_dsigmaBox_strange196 (double x) const |
| const double | getIntegrand_dsigmaBox_strange200 (double x) const |
| const double | getIntegrand_dsigmaBox_strange202 (double x) const |
| const double | getIntegrand_dsigmaBox_strange205 (double x) const |
| const double | getIntegrand_dsigmaBox_strange207 (double x) const |
| const double | getIntegrand_dsigmaBox_tau130 (double x) const |
| const double | getIntegrand_dsigmaBox_tau133 (double x) const |
| const double | getIntegrand_dsigmaBox_tau136 (double x) const |
| const double | getIntegrand_dsigmaBox_tau161 (double x) const |
| const double | getIntegrand_dsigmaBox_tau167 (double x) const |
| const double | getIntegrand_dsigmaBox_tau172 (double x) const |
| const double | getIntegrand_dsigmaBox_tau183 (double x) const |
| const double | getIntegrand_dsigmaBox_tau189 (double x) const |
| const double | getIntegrand_dsigmaBox_tau192 (double x) const |
| const double | getIntegrand_dsigmaBox_tau196 (double x) const |
| const double | getIntegrand_dsigmaBox_tau200 (double x) const |
| const double | getIntegrand_dsigmaBox_tau202 (double x) const |
| const double | getIntegrand_dsigmaBox_tau205 (double x) const |
| const double | getIntegrand_dsigmaBox_tau207 (double x) const |
| const double | getIntegrand_dsigmaBox_up130 (double x) const |
| const double | getIntegrand_dsigmaBox_up133 (double x) const |
| const double | getIntegrand_dsigmaBox_up136 (double x) const |
| const double | getIntegrand_dsigmaBox_up161 (double x) const |
| const double | getIntegrand_dsigmaBox_up167 (double x) const |
| const double | getIntegrand_dsigmaBox_up172 (double x) const |
| const double | getIntegrand_dsigmaBox_up183 (double x) const |
| const double | getIntegrand_dsigmaBox_up189 (double x) const |
| const double | getIntegrand_dsigmaBox_up192 (double x) const |
| const double | getIntegrand_dsigmaBox_up196 (double x) const |
| const double | getIntegrand_dsigmaBox_up200 (double x) const |
| const double | getIntegrand_dsigmaBox_up202 (double x) const |
| const double | getIntegrand_dsigmaBox_up205 (double x) const |
| const double | getIntegrand_dsigmaBox_up207 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom130 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom133 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom136 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom161 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom167 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom172 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom183 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom189 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom192 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom196 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom200 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom202 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom205 (double x) const |
| const double | getIntegrand_sigmaWithISR_bottom207 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm130 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm133 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm136 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm161 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm167 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm172 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm183 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm189 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm192 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm196 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm200 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm202 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm205 (double x) const |
| const double | getIntegrand_sigmaWithISR_charm207 (double x) const |
| const double | getIntegrand_sigmaWithISR_down130 (double x) const |
| const double | getIntegrand_sigmaWithISR_down133 (double x) const |
| const double | getIntegrand_sigmaWithISR_down136 (double x) const |
| const double | getIntegrand_sigmaWithISR_down161 (double x) const |
| const double | getIntegrand_sigmaWithISR_down167 (double x) const |
| const double | getIntegrand_sigmaWithISR_down172 (double x) const |
| const double | getIntegrand_sigmaWithISR_down183 (double x) const |
| const double | getIntegrand_sigmaWithISR_down189 (double x) const |
| const double | getIntegrand_sigmaWithISR_down192 (double x) const |
| const double | getIntegrand_sigmaWithISR_down196 (double x) const |
| const double | getIntegrand_sigmaWithISR_down200 (double x) const |
| const double | getIntegrand_sigmaWithISR_down202 (double x) const |
| const double | getIntegrand_sigmaWithISR_down205 (double x) const |
| const double | getIntegrand_sigmaWithISR_down207 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu130 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu136 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu161 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu172 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu183 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu189 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu192 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu196 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu200 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu202 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu205 (double x) const |
| const double | getIntegrand_sigmaWithISR_mu207 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange130 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange133 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange136 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange161 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange167 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange172 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange183 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange189 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange192 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange196 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange200 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange202 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange205 (double x) const |
| const double | getIntegrand_sigmaWithISR_strange207 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau130 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau136 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau161 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau172 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau183 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau189 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau192 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau196 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau200 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau202 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau205 (double x) const |
| const double | getIntegrand_sigmaWithISR_tau207 (double x) const |
| const double | getIntegrand_sigmaWithISR_up130 (double x) const |
| const double | getIntegrand_sigmaWithISR_up133 (double x) const |
| const double | getIntegrand_sigmaWithISR_up136 (double x) const |
| const double | getIntegrand_sigmaWithISR_up161 (double x) const |
| const double | getIntegrand_sigmaWithISR_up167 (double x) const |
| const double | getIntegrand_sigmaWithISR_up172 (double x) const |
| const double | getIntegrand_sigmaWithISR_up183 (double x) const |
| const double | getIntegrand_sigmaWithISR_up189 (double x) const |
| const double | getIntegrand_sigmaWithISR_up192 (double x) const |
| const double | getIntegrand_sigmaWithISR_up196 (double x) const |
| const double | getIntegrand_sigmaWithISR_up200 (double x) const |
| const double | getIntegrand_sigmaWithISR_up202 (double x) const |
| const double | getIntegrand_sigmaWithISR_up205 (double x) const |
| const double | getIntegrand_sigmaWithISR_up207 (double x) const |
| const double | Integrand_AFBnumeratorWithISR_l (double x, const QCD::lepton l_flavor, const double s) const |
| const double | Integrand_AFBnumeratorWithISR_q (double x, const QCD::quark q_flavor, const double s) const |
| const double | Integrand_dsigmaBox_l (double cosTheta, const QCD::lepton l_flavor, const double s) const |
| const double | Integrand_dsigmaBox_q (double cosTheta, const QCD::quark q_flavor, const double s) const |
| const double | Integrand_sigmaWithISR_l (double x, const QCD::lepton l_flavor, const double s) const |
| const double | Integrand_sigmaWithISR_q (double x, const QCD::quark q_flavor, const double s) const |
| double | m_q (const QCD::quark q, const double mu, const orders order=FULLNLO) const |
| double | RAq (const QCD::quark q) const |
| The radiator factor associated with the final-state QED and QCD corrections to the the axial-vector-current interactions, \(R_A^q(M_Z^2)\). More... | |
| double | resumKappaZ (const double DeltaRho[orders_EW_size], const double deltaKappa_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const |
| A method to compute the real part of the effetvive coupling \(\kappa_Z^f\) from \(\Delta\rho\), \(\delta\rho_{\rm rem}^{f}\) and \(\Delta r_{\mathrm{rem}}\). More... | |
| double | resumMw (const double Mw_i, const double DeltaRho[orders_EW_size], const double DeltaR_rem[orders_EW_size]) const |
| A method to compute the \(W\)-boson mass from \(\Delta\rho\) and \(\Delta r_{\mathrm{rem}}\). More... | |
| double | resumRhoZ (const double DeltaRho[orders_EW_size], const double deltaRho_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const |
| A method to compute the real part of the effective coupling \(\rho_Z^f\) from \(\Delta\rho\), \(\delta\rho_{\rm rem}^{f}\) and \(\Delta r_{\mathrm{rem}}\). More... | |
| double | RVh () const |
| The singlet vector corrections to the hadronic \(Z\)-boson width, denoted as \(R_V^h\). More... | |
| double | RVq (const QCD::quark q) const |
| The radiator factor associated with the final-state QED and QCD corrections to the the vector-current interactions, \(R_V^q(M_Z^2)\). More... | |
| double | SchemeToDouble (const std::string scheme) const |
| A method to convert a given scheme name in string form into a floating-point number with double precision. More... | |
| const double | sigma_NoISR_l (const QCD::lepton l_flavor, const double s) const |
| const double | sigma_NoISR_q (const QCD::quark q_flavor, const double s) const |
| double | taub () const |
| Top-mass corrections to the \(Zb\bar{b}\) vertex, denoted by \(\tau_b\). More... | |
| Protected Member Functions inherited from QCD | |
| const double | MassOfNf (int nf) const |
| The Mbar mass of the heaviest quark in the theory with Nf active flavour. More... | |
Protected Attributes | |
| double | ai2G |
| double | ai3G |
| double | aiA |
| double | aiB |
| double | aiG |
| double | aiH |
| double | aiHB |
| double | aiHd |
| double | aiHe |
| double | aiHL |
| double | aiHQ |
| double | aiHu |
| double | aiHW |
| double | aipHL |
| double | aipHQ |
| double | aiT |
| double | aiu |
| double | aiuG |
| double | aiWW |
| double | aleMz |
| The em constant at Mz. More... | |
| double | BrHexo |
| The branching ratio of exotic (not invisible) Higgs decays. More... | |
| double | BrHinv |
| The branching ratio of invisible Higgs decays. More... | |
| double | C1Htotal |
| The C1 coefficient controlling the H^3 corrections to the total Higgs width from the Higgs trilinear coupling. More... | |
| double | C2B |
| The dimension-6 operator coefficient \(C_{2W}\). More... | |
| double | C2BS |
| The dimension-6 operator coefficient \(C_{2W}^{SILH}\). More... | |
| double | C2W |
| The dimension-6 operator coefficient \(C_{2B}\). More... | |
| double | C2WS |
| The dimension-6 operator coefficient \(C_{2B}^{SILH}\). More... | |
| double | cAsch |
| double | CDB |
| The dimension-6 operator coefficient \(C_{DB}\). More... | |
| double | CdB_11i |
| The dimension-6 operator coefficient \((C_{dB})_{11}\) (imaginary part). More... | |
| double | CdB_11r |
| The dimension-6 operator coefficient \((C_{dB})_{11}\) (real part). More... | |
| double | CdB_12i |
| The dimension-6 operator coefficient \((C_{dB})_{12}\) (imaginary part). More... | |
| double | CdB_12r |
| The dimension-6 operator coefficient \((C_{dB})_{12}\) (real part). More... | |
| double | CdB_13i |
| The dimension-6 operator coefficient \((C_{dB})_{13}\) (imaginary part). More... | |
| double | CdB_13r |
| The dimension-6 operator coefficient \((C_{dB})_{13}\) (real part). More... | |
| double | CdB_22i |
| The dimension-6 operator coefficient \((C_{dB})_{22}\) (imaginary part). More... | |
| double | CdB_22r |
| The dimension-6 operator coefficient \((C_{dB})_{22}\) (real part). More... | |
| double | CdB_23i |
| The dimension-6 operator coefficient \((C_{dB})_{23}\) (imaginary part). More... | |
| double | CdB_23r |
| The dimension-6 operator coefficient \((C_{dB})_{23}\) (real part). More... | |
| double | CdB_33i |
| The dimension-6 operator coefficient \((C_{dB})_{33}\) (imaginary part). More... | |
| double | CdB_33r |
| The dimension-6 operator coefficient \((C_{dB})_{33}\) (real part). More... | |
| double | CdG_11i |
| The dimension-6 operator coefficient \((C_{dG})_{11}\) (imaginary part). More... | |
| double | CdG_11r |
| The dimension-6 operator coefficient \((C_{dG})_{11}\) (real part). More... | |
| double | CdG_12i |
| The dimension-6 operator coefficient \((C_{dG})_{12}\) (imaginary part). More... | |
| double | CdG_12r |
| The dimension-6 operator coefficient \((C_{dG})_{12}\) (real part). More... | |
| double | CdG_13i |
| The dimension-6 operator coefficient \((C_{dG})_{13}\) (imaginary part). More... | |
| double | CdG_13r |
| The dimension-6 operator coefficient \((C_{dG})_{13}\) (real part). More... | |
| double | CdG_22i |
| The dimension-6 operator coefficient \((C_{dG})_{22}\) (imaginary part). More... | |
| double | CdG_22r |
| The dimension-6 operator coefficient \((C_{dG})_{22}\) (real part). More... | |
| double | CdG_23i |
| The dimension-6 operator coefficient \((C_{dG})_{23}\) (imaginary part). More... | |
| double | CdG_23r |
| The dimension-6 operator coefficient \((C_{dG})_{23}\) (real part). More... | |
| double | CdG_33i |
| The dimension-6 operator coefficient \((C_{dG})_{33}\) (imaginary part). More... | |
| double | CdG_33r |
| The dimension-6 operator coefficient \((C_{dG})_{33}\) (real part). More... | |
| double | CdH_11i |
| The dimension-6 operator coefficient \((C_{dH})_{11}\) (imaginary part). More... | |
| double | CdH_11r |
| The dimension-6 operator coefficient \((C_{dH})_{11}\) (real part). More... | |
| double | CdH_12i |
| The dimension-6 operator coefficient \((C_{dH})_{12}\) (imaginary part). More... | |
| double | CdH_12r |
| The dimension-6 operator coefficient \((C_{dH})_{12}\) (real part). More... | |
| double | CdH_13i |
| The dimension-6 operator coefficient \((C_{dH})_{13}\) (imaginary part). More... | |
| double | CdH_13r |
| The dimension-6 operator coefficient \((C_{dH})_{13}\) (real part). More... | |
| double | CdH_22i |
| The dimension-6 operator coefficient \((C_{dH})_{22}\) (imaginary part). More... | |
| double | CdH_22r |
| The dimension-6 operator coefficient \((C_{dH})_{22}\) (real part). More... | |
| double | CdH_23i |
| The dimension-6 operator coefficient \((C_{dH})_{23}\) (imaginary part). More... | |
| double | CdH_23r |
| The dimension-6 operator coefficient \((C_{dH})_{23}\) (real part). More... | |
| double | CdH_33i |
| The dimension-6 operator coefficient \((C_{dH})_{33}\) (imaginary part). More... | |
| double | CdH_33r |
| The dimension-6 operator coefficient \((C_{dH})_{33}\) (real part). More... | |
| double | CDHB |
| The dimension-6 operator coefficient \(C_{DHB}\). More... | |
| double | CDHW |
| The dimension-6 operator coefficient \(C_{DHW}\). More... | |
| double | CDW |
| The dimension-6 operator coefficient \(C_{DW}\). More... | |
| double | CdW_11i |
| The dimension-6 operator coefficient \((C_{dW})_{11}\) (imaginary part). More... | |
| double | CdW_11r |
| The dimension-6 operator coefficient \((C_{dW})_{11}\) (real part). More... | |
| double | CdW_12i |
| The dimension-6 operator coefficient \((C_{dW})_{12}\) (imaginary part). More... | |
| double | CdW_12r |
| The dimension-6 operator coefficient \((C_{dW})_{12}\) (real part). More... | |
| double | CdW_13i |
| The dimension-6 operator coefficient \((C_{dW})_{13}\) (imaginary part). More... | |
| double | CdW_13r |
| The dimension-6 operator coefficient \((C_{dW})_{13}\) (real part). More... | |
| double | CdW_22i |
| The dimension-6 operator coefficient \((C_{dW})_{22}\) (imaginary part). More... | |
| double | CdW_22r |
| The dimension-6 operator coefficient \((C_{dW})_{22}\) (real part). More... | |
| double | CdW_23i |
| The dimension-6 operator coefficient \((C_{dW})_{23}\) (imaginary part). More... | |
| double | CdW_23r |
| The dimension-6 operator coefficient \((C_{dW})_{23}\) (real part). More... | |
| double | CdW_33i |
| The dimension-6 operator coefficient \((C_{dW})_{33}\) (imaginary part). More... | |
| double | CdW_33r |
| The dimension-6 operator coefficient \((C_{dW})_{33}\) (real part). More... | |
| double | CeB_11i |
| The dimension-6 operator coefficient \((C_{eB})_{11}\) (imaginary part). More... | |
| double | CeB_11r |
| The dimension-6 operator coefficient \((C_{eB})_{11}\) (real part). More... | |
| double | CeB_12i |
| The dimension-6 operator coefficient \((C_{eB})_{12}\) (imaginary part). More... | |
| double | CeB_12r |
| The dimension-6 operator coefficient \((C_{eB})_{12}\) (real part). More... | |
| double | CeB_13i |
| The dimension-6 operator coefficient \((C_{eB})_{13}\) (imaginary part). More... | |
| double | CeB_13r |
| The dimension-6 operator coefficient \((C_{eB})_{13}\) (real part). More... | |
| double | CeB_22i |
| The dimension-6 operator coefficient \((C_{eB})_{22}\) (imaginary part). More... | |
| double | CeB_22r |
| The dimension-6 operator coefficient \((C_{eB})_{22}\) (real part). More... | |
| double | CeB_23i |
| The dimension-6 operator coefficient \((C_{eB})_{23}\) (imaginary part). More... | |
| double | CeB_23r |
| The dimension-6 operator coefficient \((C_{eB})_{23}\) (real part). More... | |
| double | CeB_33i |
| The dimension-6 operator coefficient \((C_{eB})_{33}\) (imaginary part). More... | |
| double | CeB_33r |
| The dimension-6 operator coefficient \((C_{eB})_{33}\) (real part). More... | |
| double | Ced_1111 |
| double | Ced_1122 |
| double | Ced_1123 |
| double | Ced_1132 |
| double | Ced_1133 |
| double | Ced_2211 |
| double | Ced_2223 |
| double | Ced_2232 |
| double | Ced_3311 |
| double | Ced_3323 |
| double | Ced_3332 |
| double | Cee_1111 |
| double | Cee_1122 |
| double | Cee_1133 |
| double | Cee_2211 |
| double | Cee_3311 |
| double | CeH_11i |
| The dimension-6 operator coefficient \((C_{eH})_{11}\) (imaginary part). More... | |
| double | CeH_11r |
| The dimension-6 operator coefficient \((C_{eH})_{11}\) (real part). More... | |
| double | CeH_12i |
| The dimension-6 operator coefficient \((C_{eH})_{12}\) (imaginary part). More... | |
| double | CeH_12r |
| The dimension-6 operator coefficient \((C_{eH})_{12}\) (real part). More... | |
| double | CeH_13i |
| The dimension-6 operator coefficient \((C_{eH})_{13}\) (imaginary part). More... | |
| double | CeH_13r |
| The dimension-6 operator coefficient \((C_{eH})_{13}\) (real part). More... | |
| double | CeH_22i |
| The dimension-6 operator coefficient \((C_{eH})_{22}\) (imaginary part). More... | |
| double | CeH_22r |
| The dimension-6 operator coefficient \((C_{eH})_{22}\) (real part). More... | |
| double | CeH_23i |
| The dimension-6 operator coefficient \((C_{eH})_{23}\) (imaginary part). More... | |
| double | CeH_23r |
| The dimension-6 operator coefficient \((C_{eH})_{23}\) (real part). More... | |
| double | CeH_33i |
| The dimension-6 operator coefficient \((C_{eH})_{33}\) (imaginary part). More... | |
| double | CeH_33r |
| The dimension-6 operator coefficient \((C_{eH})_{33}\) (real part). More... | |
| double | Ceu_1111 |
| double | Ceu_1122 |
| double | Ceu_1133 |
| double | Ceu_2211 |
| double | Ceu_2233 |
| double | Ceu_3311 |
| double | CeW_11i |
| The dimension-6 operator coefficient \((C_{eW})_{11}\) (imaginary part). More... | |
| double | CeW_11r |
| The dimension-6 operator coefficient \((C_{eW})_{11}\) (real part). More... | |
| double | CeW_12i |
| The dimension-6 operator coefficient \((C_{eW})_{12}\) (imaginary part). More... | |
| double | CeW_12r |
| The dimension-6 operator coefficient \((C_{eW})_{12}\) (real part). More... | |
| double | CeW_13i |
| The dimension-6 operator coefficient \((C_{eW})_{13}\) (imaginary part). More... | |
| double | CeW_13r |
| The dimension-6 operator coefficient \((C_{eW})_{13}\) (real part). More... | |
| double | CeW_22i |
| The dimension-6 operator coefficient \((C_{eW})_{22}\) (imaginary part). More... | |
| double | CeW_22r |
| The dimension-6 operator coefficient \((C_{eW})_{22}\) (real part). More... | |
| double | CeW_23i |
| The dimension-6 operator coefficient \((C_{eW})_{23}\) (imaginary part). More... | |
| double | CeW_23r |
| The dimension-6 operator coefficient \((C_{eW})_{23}\) (real part). More... | |
| double | CeW_33i |
| The dimension-6 operator coefficient \((C_{eW})_{33}\) (imaginary part). More... | |
| double | CeW_33r |
| The dimension-6 operator coefficient \((C_{eW})_{33}\) (real part). More... | |
| double | CG |
| The dimension-6 operator coefficient \(C_{G}\). More... | |
| double | CH |
| The dimension-6 operator coefficient \(C_{H}\). More... | |
| double | CHB |
| The dimension-6 operator coefficient \(C_{HB}\). More... | |
| double | CHbox |
| The dimension-6 operator coefficient \(C_{H\Box}\). More... | |
| double | CHD |
| The dimension-6 operator coefficient \(C_{HD}\). More... | |
| double | CHd_11 |
| The dimension-6 operator coefficient \((C_{Hd})_{11}\). More... | |
| double | CHd_12i |
| The dimension-6 operator coefficient \((C_{Hd})_{12}\) (imaginary part). More... | |
| double | CHd_12r |
| The dimension-6 operator coefficient \((C_{Hd})_{12}\) (real part). More... | |
| double | CHd_13i |
| The dimension-6 operator coefficient \((C_{Hd})_{13}\) (imaginary part). More... | |
| double | CHd_13r |
| The dimension-6 operator coefficient \((C_{Hd})_{13}\) (real part). More... | |
| double | CHd_22 |
| The dimension-6 operator coefficient \((C_{Hd})_{22}\). More... | |
| double | CHd_23i |
| The dimension-6 operator coefficient \((C_{Hd})_{23}\) (imaginary part). More... | |
| double | CHd_23r |
| The dimension-6 operator coefficient \((C_{Hd})_{23}\) (real part). More... | |
| double | CHd_33 |
| The dimension-6 operator coefficient \((C_{Hd})_{33}\). More... | |
| double | CHdhat |
| double | CHe_11 |
| The dimension-6 operator coefficient \((C_{He})_{11}\). More... | |
| double | CHe_12i |
| The dimension-6 operator coefficient \((C_{He})_{12}\) (imaginary part). More... | |
| double | CHe_12r |
| The dimension-6 operator coefficient \((C_{He})_{12}\) (real part). More... | |
| double | CHe_13i |
| The dimension-6 operator coefficient \((C_{He})_{13}\) (imaginary part). More... | |
| double | CHe_13r |
| The dimension-6 operator coefficient \((C_{He})_{13}\) (real part). More... | |
| double | CHe_22 |
| The dimension-6 operator coefficient \((C_{He})_{22}\). More... | |
| double | CHe_23i |
| The dimension-6 operator coefficient \((C_{He})_{23}\) (imaginary part). More... | |
| double | CHe_23r |
| The dimension-6 operator coefficient \((C_{He})_{23}\) (real part). More... | |
| double | CHe_33 |
| The dimension-6 operator coefficient \((C_{He})_{33}\). More... | |
| double | CHehat |
| double | CHG |
| The dimension-6 operator coefficient \(C_{HG}\). More... | |
| double | CHL1_11 |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{11}\). More... | |
| double | CHL1_12i |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (imaginary part). More... | |
| double | CHL1_12r |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (real part). More... | |
| double | CHL1_13i |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (imaginary part). More... | |
| double | CHL1_13r |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (real part). More... | |
| double | CHL1_22 |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{22}\). More... | |
| double | CHL1_23i |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (imaginary part). More... | |
| double | CHL1_23r |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (real part). More... | |
| double | CHL1_33 |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{33}\). More... | |
| double | CHL1hat |
| double | CHL3_11 |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{11}\). More... | |
| double | CHL3_12i |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part). More... | |
| double | CHL3_12r |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part). More... | |
| double | CHL3_13i |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part). More... | |
| double | CHL3_13r |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part). More... | |
| double | CHL3_22 |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{22}\). More... | |
| double | CHL3_23i |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part). More... | |
| double | CHL3_23r |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part). More... | |
| double | CHL3_33 |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{33}\). More... | |
| double | CHL3hat |
| double | CHQ1_11 |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{11}\). More... | |
| double | CHQ1_12i |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (imaginary part). More... | |
| double | CHQ1_12r |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (real part). More... | |
| double | CHQ1_13i |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (imaginary part). More... | |
| double | CHQ1_13r |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (real part). More... | |
| double | CHQ1_22 |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{22}\). More... | |
| double | CHQ1_23i |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (imaginary part). More... | |
| double | CHQ1_23r |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (real part). More... | |
| double | CHQ1_33 |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{33}\). More... | |
| double | CHQ1hat |
| double | CHQ3_11 |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{11}\). More... | |
| double | CHQ3_12i |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (imaginary part). More... | |
| double | CHQ3_12r |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (real part). More... | |
| double | CHQ3_13i |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (imaginary part). More... | |
| double | CHQ3_13r |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (real part). More... | |
| double | CHQ3_22 |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{22}\). More... | |
| double | CHQ3_23i |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (imaginary part). More... | |
| double | CHQ3_23r |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (real part). More... | |
| double | CHQ3_33 |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{33}\). More... | |
| double | CHQ3hat |
| double | cHSM |
| Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes. More... | |
| double | CHu_11 |
| The dimension-6 operator coefficient \((C_{Hu})_{11}\). More... | |
| double | CHu_12i |
| The dimension-6 operator coefficient \((C_{Hu})_{12}\) (imaginary part). More... | |
| double | CHu_12r |
| The dimension-6 operator coefficient \((C_{Hu})_{12}\) (real part). More... | |
| double | CHu_13i |
| The dimension-6 operator coefficient \((C_{Hu})_{13}\) (imaginary part). More... | |
| double | CHu_13r |
| The dimension-6 operator coefficient \((C_{Hu})_{13}\) (real part). More... | |
| double | CHu_22 |
| The dimension-6 operator coefficient \((C_{Hu})_{22}\). More... | |
| double | CHu_23i |
| The dimension-6 operator coefficient \((C_{Hu})_{23}\) (imaginary part). More... | |
| double | CHu_23r |
| The dimension-6 operator coefficient \((C_{Hu})_{23}\) (real part). More... | |
| double | CHu_33 |
| The dimension-6 operator coefficient \((C_{Hu})_{33}\). More... | |
| double | CHud_11i |
| The dimension-6 operator coefficient \((C_{Hud})_{11}\) (imaginary part). More... | |
| double | CHud_11r |
| The dimension-6 operator coefficient \((C_{Hud})_{11}\) (real part). More... | |
| double | CHud_12i |
| The dimension-6 operator coefficient \((C_{Hud})_{12}\) (imaginary part). More... | |
| double | CHud_12r |
| The dimension-6 operator coefficient \((C_{Hud})_{12}\) (real part). More... | |
| double | CHud_13i |
| The dimension-6 operator coefficient \((C_{Hud})_{13}\) (imaginary part). More... | |
| double | CHud_13r |
| The dimension-6 operator coefficient \((C_{Hud})_{13}\) (real part). More... | |
| double | CHud_22i |
| The dimension-6 operator coefficient \((C_{Hud})_{22}\) (imaginary part). More... | |
| double | CHud_22r |
| The dimension-6 operator coefficient \((C_{Hud})_{22}\) (real part). More... | |
| double | CHud_23i |
| The dimension-6 operator coefficient \((C_{Hud})_{23}\) (imaginary part). More... | |
| double | CHud_23r |
| The dimension-6 operator coefficient \((C_{Hud})_{23}\) (real part). More... | |
| double | CHud_33i |
| The dimension-6 operator coefficient \((C_{Hud})_{33}\) (imaginary part). More... | |
| double | CHud_33r |
| The dimension-6 operator coefficient \((C_{Hud})_{33}\) (real part). More... | |
| double | CHuhat |
| double | CHW |
| The dimension-6 operator coefficient \(C_{HW}\). More... | |
| double | CHWB |
| The dimension-6 operator coefficient \(C_{HWB}\). More... | |
| double | CHWHB_gaga |
| The combination of dimension-6 operator coefficients entering in \(\delta_{AA}\): \(s_W^2 C_{HW} + c_W^2 C_{HW}\). More... | |
| double | CHWHB_gagaorth |
| The combination of dimension-6 operator coefficients \(-c_W^2 C_{HW} + s_W^2 C_{HW}\). More... | |
| double | CHWpCHB |
| double | CidH_11r |
| double | CidH_22r |
| double | CidH_33r |
| double | CiDHB |
| double | CiDHW |
| double | CieH_11r |
| double | CieH_22r |
| double | CieH_33r |
| double | CiG |
| double | CiH |
| double | CiHB |
| double | CiHbox |
| double | CiHD |
| double | CiHd_11 |
| double | CiHd_22 |
| double | CiHd_33 |
| double | CiHe_11 |
| double | CiHe_22 |
| double | CiHe_33 |
| double | CiHG |
| double | CiHL1_11 |
| double | CiHL1_22 |
| double | CiHL1_33 |
| double | CiHL3_11 |
| double | CiHL3_22 |
| double | CiHL3_33 |
| double | CiHQ1_11 |
| double | CiHQ1_22 |
| double | CiHQ1_33 |
| double | CiHQ3_11 |
| double | CiHQ3_22 |
| double | CiHQ3_33 |
| double | CiHu_11 |
| double | CiHu_22 |
| double | CiHu_33 |
| double | CiHW |
| double | CiHWB |
| double | CiLL_1221 |
| double | CiLL_2112 |
| double | CiuB_11r |
| double | CiuB_22r |
| double | CiuB_33r |
| double | CiuG_11r |
| double | CiuG_22r |
| double | CiuG_33r |
| double | CiuH_11r |
| double | CiuH_22r |
| double | CiuH_33r |
| double | CiuW_11r |
| double | CiuW_22r |
| double | CiuW_33r |
| double | CiW |
| double | CLd_1111 |
| double | CLd_1122 |
| double | CLd_1123 |
| double | CLd_1132 |
| double | CLd_1133 |
| double | CLd_2211 |
| double | CLd_2223 |
| double | CLd_2232 |
| double | CLd_3311 |
| double | CLd_3323 |
| double | CLd_3332 |
| double | CLe_1111 |
| double | CLe_1122 |
| double | CLe_1133 |
| double | CLe_2211 |
| double | CLe_3311 |
| double | CLedQ_11 |
| double | CLedQ_22 |
| double | cLH3d62 |
| Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions modifying the Higgs trilinear coupling (Quadratic terms). More... | |
| double | cLHd6 |
| Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions. More... | |
| double | CLL_1111 |
| double | CLL_1122 |
| double | CLL_1133 |
| double | CLL_1221 |
| double | CLL_1331 |
| double | CLL_2112 |
| double | CLL_2211 |
| double | CLL_3113 |
| double | CLL_3311 |
| double | CLLhat |
| double | CLQ1_1111 |
| double | CLQ1_1122 |
| double | CLQ1_1123 |
| double | CLQ1_1132 |
| double | CLQ1_1133 |
| double | CLQ1_1221 |
| double | CLQ1_1331 |
| double | CLQ1_2112 |
| double | CLQ1_2211 |
| double | CLQ1_2223 |
| double | CLQ1_2232 |
| double | CLQ1_3113 |
| double | CLQ1_3311 |
| double | CLQ1_3323 |
| double | CLQ1_3332 |
| double | CLQ3_1111 |
| double | CLQ3_1122 |
| double | CLQ3_1123 |
| double | CLQ3_1132 |
| double | CLQ3_1133 |
| double | CLQ3_1221 |
| double | CLQ3_1331 |
| double | CLQ3_2112 |
| double | CLQ3_2211 |
| double | CLQ3_2223 |
| double | CLQ3_2232 |
| double | CLQ3_3113 |
| double | CLQ3_3311 |
| double | CLQ3_3323 |
| double | CLQ3_3332 |
| double | CLu_1111 |
| double | CLu_1122 |
| double | CLu_1133 |
| double | CLu_2211 |
| double | CLu_2233 |
| double | CLu_3311 |
| double | CpLedQ_11 |
| double | CpLedQ_22 |
| double | CQd1_3311 |
| double | CQd1_3322 |
| double | CQd1_3333 |
| double | CQd8_3311 |
| double | CQd8_3322 |
| double | CQd8_3333 |
| double | CQe_1111 |
| double | CQe_1122 |
| double | CQe_1133 |
| double | CQe_2211 |
| double | CQe_2311 |
| double | CQe_2322 |
| double | CQe_2333 |
| double | CQe_3211 |
| double | CQe_3222 |
| double | CQe_3233 |
| double | CQe_3311 |
| double | CQQ1_1133 |
| double | CQQ1_1331 |
| double | CQQ1_2233 |
| double | CQQ1_2332 |
| double | CQQ1_3333 |
| double | CQQ3_1133 |
| double | CQQ3_1331 |
| double | CQQ3_2233 |
| double | CQQ3_2332 |
| double | CQQ3_3333 |
| double | CQu1_1133 |
| double | CQu1_2233 |
| double | CQu1_3311 |
| double | CQu1_3322 |
| double | CQu1_3333 |
| double | CQu8_1133 |
| double | CQu8_2233 |
| double | CQu8_3311 |
| double | CQu8_3322 |
| double | CQu8_3333 |
| double | CQuQd1_3333 |
| double | CQuQd8_3333 |
| double | cRGE |
| Parameter to control the inclusion of log-enhanced contributions via RG effects. If activated then it takes the value multiplying the anomalous dimension: \(-\log(\Lambda/\mu)/16 \pi^2 \Lambda^2\). More... | |
| double | cRGEon |
| Another parameter to control the inclusion of log-enhanced contributions via RG effects. It multiplies the logarithmic contribution to some observables, so it takes values 0/1 to deactivate/activate the log terms. More... | |
| double | CT |
| The dimension-6 operator coefficient \(C_{T}\). More... | |
| double | CuB_11i |
| The dimension-6 operator coefficient \((C_{uB})_{11}\) (imaginary part). More... | |
| double | CuB_11r |
| The dimension-6 operator coefficient \((C_{uB})_{11}\) (real part). More... | |
| double | CuB_12i |
| The dimension-6 operator coefficient \((C_{uB})_{12}\) (imaginary part). More... | |
| double | CuB_12r |
| The dimension-6 operator coefficient \((C_{uB})_{12}\) (real part). More... | |
| double | CuB_13i |
| The dimension-6 operator coefficient \((C_{uB})_{13}\) (imaginary part). More... | |
| double | CuB_13r |
| The dimension-6 operator coefficient \((C_{uB})_{13}\) (real part). More... | |
| double | CuB_22i |
| The dimension-6 operator coefficient \((C_{uB})_{22}\) (imaginary part). More... | |
| double | CuB_22r |
| The dimension-6 operator coefficient \((C_{uB})_{22}\) (real part). More... | |
| double | CuB_23i |
| The dimension-6 operator coefficient \((C_{uB})_{23}\) (imaginary part). More... | |
| double | CuB_23r |
| The dimension-6 operator coefficient \((C_{uB})_{23}\) (real part). More... | |
| double | CuB_33i |
| The dimension-6 operator coefficient \((C_{uB})_{33}\) (imaginary part). More... | |
| double | CuB_33r |
| The dimension-6 operator coefficient \((C_{uB})_{33}\) (real part). More... | |
| double | Cud1_3311 |
| double | Cud1_3322 |
| double | Cud1_3333 |
| double | Cud8_3311 |
| double | Cud8_3322 |
| double | Cud8_3333 |
| double | CuG_11i |
| The dimension-6 operator coefficient \((C_{uG})_{11}\) (imaginary part). More... | |
| double | CuG_11r |
| The dimension-6 operator coefficient \((C_{uG})_{11}\) (real part). More... | |
| double | CuG_12i |
| The dimension-6 operator coefficient \((C_{uG})_{12}\) (imaginary part). More... | |
| double | CuG_12r |
| The dimension-6 operator coefficient \((C_{uG})_{12}\) (real part). More... | |
| double | CuG_13i |
| The dimension-6 operator coefficient \((C_{uG})_{13}\) (imaginary part). More... | |
| double | CuG_13r |
| The dimension-6 operator coefficient \((C_{uG})_{13}\) (real part). More... | |
| double | CuG_22i |
| The dimension-6 operator coefficient \((C_{uG})_{22}\) (imaginary part). More... | |
| double | CuG_22r |
| The dimension-6 operator coefficient \((C_{uG})_{22}\) (real part). More... | |
| double | CuG_23i |
| The dimension-6 operator coefficient \((C_{uG})_{23}\) (imaginary part). More... | |
| double | CuG_23r |
| The dimension-6 operator coefficient \((C_{uG})_{23}\) (real part). More... | |
| double | CuG_33i |
| The dimension-6 operator coefficient \((C_{uG})_{33}\) (imaginary part). More... | |
| double | CuG_33r |
| The dimension-6 operator coefficient \((C_{uG})_{33}\) (real part). More... | |
| double | CuH_11i |
| The dimension-6 operator coefficient \((C_{uH})_{11}\) (imaginary part). More... | |
| double | CuH_11r |
| The dimension-6 operator coefficient \((C_{uH})_{11}\) (real part). More... | |
| double | CuH_12i |
| The dimension-6 operator coefficient \((C_{uH})_{12}\) (imaginary part). More... | |
| double | CuH_12r |
| The dimension-6 operator coefficient \((C_{uH})_{12}\) (real part). More... | |
| double | CuH_13i |
| The dimension-6 operator coefficient \((C_{uH})_{13}\) (imaginary part). More... | |
| double | CuH_13r |
| The dimension-6 operator coefficient \((C_{uH})_{13}\) (real part). More... | |
| double | CuH_22i |
| The dimension-6 operator coefficient \((C_{uH})_{22}\) (imaginary part). More... | |
| double | CuH_22r |
| The dimension-6 operator coefficient \((C_{uH})_{22}\) (real part). More... | |
| double | CuH_23i |
| The dimension-6 operator coefficient \((C_{uH})_{23}\) (imaginary part). More... | |
| double | CuH_23r |
| The dimension-6 operator coefficient \((C_{uH})_{23}\) (real part). More... | |
| double | CuH_33i |
| The dimension-6 operator coefficient \((C_{uH})_{33}\) (imaginary part). More... | |
| double | CuH_33r |
| The dimension-6 operator coefficient \((C_{uH})_{33}\) (real part). More... | |
| double | Cuu_1133 |
| double | Cuu_1331 |
| double | Cuu_2233 |
| double | Cuu_2332 |
| double | Cuu_3333 |
| double | CuW_11i |
| The dimension-6 operator coefficient \((C_{uW})_{11}\) (imaginary part). More... | |
| double | CuW_11r |
| The dimension-6 operator coefficient \((C_{uW})_{11}\) (real part). More... | |
| double | CuW_12i |
| The dimension-6 operator coefficient \((C_{uW})_{12}\) (imaginary part). More... | |
| double | CuW_12r |
| The dimension-6 operator coefficient \((C_{uW})_{12}\) (real part). More... | |
| double | CuW_13i |
| The dimension-6 operator coefficient \((C_{uW})_{13}\) (imaginary part). More... | |
| double | CuW_13r |
| The dimension-6 operator coefficient \((C_{uW})_{13}\) (real part). More... | |
| double | CuW_22i |
| The dimension-6 operator coefficient \((C_{uW})_{22}\) (imaginary part). More... | |
| double | CuW_22r |
| The dimension-6 operator coefficient \((C_{uW})_{22}\) (real part). More... | |
| double | CuW_23i |
| The dimension-6 operator coefficient \((C_{uW})_{23}\) (imaginary part). More... | |
| double | CuW_23r |
| The dimension-6 operator coefficient \((C_{uW})_{23}\) (real part). More... | |
| double | CuW_33i |
| The dimension-6 operator coefficient \((C_{uW})_{33}\) (imaginary part). More... | |
| double | CuW_33r |
| The dimension-6 operator coefficient \((C_{uW})_{33}\) (real part). More... | |
| double | CW |
| The dimension-6 operator coefficient \(C_{W}\). More... | |
| double | cW2_tree |
| The square of the tree level values for the cosine of the weak angle. More... | |
| double | cW_tree |
| The tree level values for the cosine of the weak angle. More... | |
| double | cWsch |
| Parameters to control the SM EW input scheme: Alpha or MW. More... | |
| double | delta_A |
| Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition for EWPO. More... | |
| double | delta_AA |
| Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition. More... | |
| double | delta_ale |
| The \(\mathcal{O}(\Lambda^{-2})\) dimension 6 correction to the electromagnetic coupling. More... | |
| double | delta_ale_2 |
| The \(\mathcal{O}(\Lambda^{-4})\) dimension 6 correction to the electromagnetic coupling. More... | |
| double | delta_AZ |
| Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition. More... | |
| double | delta_e |
| The dimension 6 correction to the electric constant parameter. More... | |
| double | delta_em |
| The relative dimension 6 correction to the QED interaction vertex. More... | |
| double | delta_g1 |
| The \(\mathcal{O}(\Lambda^{-2})\) dimension 6 correction to the \(U(1)_Y\) gauge coupling, for the Alpha-Scheme (cAsch=1, cWsch=0) or the Mw-Scheme (cAsch=0, cWsch=1). More... | |
| double | delta_g1_2 |
| The \(\mathcal{O}(\Lambda^{-4})\) dimension 6 correction to the \(U(1)_Y\) gauge coupling. More... | |
| double | delta_g2 |
| The \(\mathcal{O}(\Lambda^{-2})\) dimension 6 correction to the \(SU(2)_L\) gauge coupling, for the Alpha-Scheme (cAsch=1, cWsch=0) or the Mw-Scheme (cAsch=0, cWsch=1). More... | |
| double | delta_g2_2 |
| The \(\mathcal{O}(\Lambda^{-4})\) dimension 6 correction to the \(SU(2)_L\) gauge coupling. More... | |
| double | delta_GF |
| The dimension 6 correction to the Fermi constant, as extracted from muon decay. More... | |
| double | delta_GF_2 |
| The \(\mathcal{O}(\Lambda^{-4})\) dimension 6 correction to the Fermi constant. More... | |
| double | delta_h |
| Combinations of dimension 6 coefficients modifying the \(H\) canonical field definition. More... | |
| double | delta_MW |
| The dimension 6 correction to W mass Lagrangian parameter. More... | |
| double | delta_MZ |
| The dimension 6 correction to Z mass Lagrangian parameter. More... | |
| double | delta_Mz2 |
| The \(\mathcal{O}(\Lambda^{-2})\) dimension 6 correction to the Z-boson mass squared. More... | |
| double | delta_Mz2_2 |
| The \(\mathcal{O}(\Lambda^{-4})\) dimension 6 correction to the Z-boson mass squared. More... | |
| double | delta_QgNC |
| The dimension 6 charge correction to neutral current EW couplings. More... | |
| double | delta_sW2 |
| The dimension 6 correction to the weak mixing angle. More... | |
| double | delta_UgCC |
| The dimension 6 universal correction to charged current EW couplings. More... | |
| double | delta_UgNC |
| The dimension 6 universal correction to neutral current EW couplings. More... | |
| double | delta_v |
| The dimension 6 correction to the vev, as extracted from GF. More... | |
| double | delta_xBZ |
| The \(\mathcal{O}(\Lambda^{-2})\) dimension 6 correction to the component of the matrix that transform the gauge field \(B_{\mu}\) into \(Z_{\mu}\). More... | |
| double | delta_xBZ_2 |
| The \(\mathcal{O}(\Lambda^{-4})\) dimension 6 correction to the component of the matrix that transform the gauge field \(B_{\mu}\) into \(Z_{\mu}\). More... | |
| double | delta_xWZ |
| The \(\mathcal{O}(\Lambda^{-2})\) dimension 6 correction to the component of the matrix that transform the gauge field \(W_{\mu}^3\) into \(Z_{\mu}\). More... | |
| double | delta_xWZ_2 |
| The \(\mathcal{O}(\Lambda^{-4})\) dimension 6 correction to the component of the matrix that transform the gauge field \(W_{\mu}^3\) into \(Z_{\mu}\). More... | |
| double | delta_Z |
| Combination of dimension 6 coefficients modifying the \(Z_\mu\) canonical field definition for EWPO. More... | |
| double | delta_ZA |
| Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition for EWPO. More... | |
| double | delta_ZZ |
| Combination of dimension 6 coefficients modifying the \(Z_\mu\) canonical field definition. More... | |
| double | dg1Z |
| Independent contribution to aTGC. More... | |
| double | dGammaHTotR1 |
| double | dGammaHTotR2 |
| double | dKappaga |
| Independent contribution to aTGC. More... | |
| double | dZH |
| double | dZH1 |
| double | dZH2 |
| Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization and combinations entering in the linear and quadratic pieces. More... | |
| double | edeeWWdcint |
| Intrinsic relative theoretical error in \(e^+ e^- \to W^+ W^-\): total cross section and \(d/d\cos{\theta}\) distribution. More... | |
| double | eeettHint |
| Intrinsic relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.) More... | |
| double | eeettHpar |
| Parametric relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.) More... | |
| double | eeeWBFint |
| Intrinsic relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.) More... | |
| double | eeeWBFpar |
| Parametric relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.) More... | |
| double | eeeWWint |
| double | eeeZHint |
| Intrinsic relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.) More... | |
| double | eeeZHpar |
| Parametric relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.) More... | |
| double | eeMz |
| The em coupling at Mz. More... | |
| double | eeMz2 |
| The em coupling squared (at Mz). More... | |
| double | eepWBFint |
| Intrinsic relative theoretical error in \(e^- p \to H e^- j\) via WBF. (Assumed to be constant in energy.) More... | |
| double | eepWBFpar |
| Parametric relative theoretical error in \(e^- p \to H e^- j\) via WBF. (Assumed to be constant in energy.) More... | |
| double | eepZBFint |
| Intrinsic relative theoretical error in \(e^- p \to H e^- j\) via ZBF. (Assumed to be constant in energy.) More... | |
| double | eepZBFpar |
| Parametric relative theoretical error in \(e^- p \to H e^- j\) via ZBF. (Assumed to be constant in energy.) More... | |
| double | eggFHbb |
| double | eggFHgaga |
| double | eggFHmumu |
| Total relative theoretical error in \(gg \to H \to X\). More... | |
| double | eggFHtautau |
| double | eggFHWW |
| double | eggFHZga |
| double | eggFHZZ |
| double | eggFint |
| Intrinsic relative theoretical error in ggF production. (Assumed to be constant in energy.) More... | |
| double | eggFpar |
| Parametric relative theoretical error in ggF production. (Assumed to be constant in energy.) More... | |
| double | eHbbint |
| Intrinsic relative theoretical error in \(H \to b\bar{b}\). More... | |
| double | eHbbpar |
| Parametric relative theoretical error in \(H \to b\bar{b}\). More... | |
| double | eHccint |
| Intrinsic relative theoretical error in \(H \to c\bar{c}\). More... | |
| double | eHccpar |
| Parametric relative theoretical error in \(H \to c\bar{c}\). More... | |
| double | eHgagaint |
| Intrinsic relative theoretical error in \(H \to \gamma\gamma\). More... | |
| double | eHgagapar |
| Parametric relative theoretical error in \(H \to \gamma\gamma\). More... | |
| double | eHggint |
| Intrinsic relative theoretical error in \(H \to g g\). More... | |
| double | eHggpar |
| Parametric relative theoretical error in \(H \to g g\). More... | |
| double | eHmumuint |
| Intrinsic relative theoretical error in \(H \to \mu^+ \mu^-\). More... | |
| double | eHmumupar |
| Parametric relative theoretical error in \(H \to \mu^+ \mu^-\). More... | |
| double | eHtautauint |
| Intrinsic relative theoretical error in \(H \to \tau^+ \tau^-\). More... | |
| double | eHtautaupar |
| Parametric relative theoretical error in \(H \to \tau^+ \tau^-\). More... | |
| double | eHwidth |
| Total relative theoretical error in the Higgs width. More... | |
| double | eHWWint |
| Intrinsic relative theoretical error in \(H \to W W\). More... | |
| double | eHWWpar |
| Parametric relative theoretical error in \(H \to W W\). More... | |
| double | eHZgaint |
| Intrinsic relative theoretical error in \(H \to Z \gamma\). More... | |
| double | eHZgapar |
| Parametric relative theoretical error in \(H \to Z \gamma\). More... | |
| double | eHZZint |
| Intrinsic relative theoretical error in \(H \to Z Z\). More... | |
| double | eHZZpar |
| Parametric relative theoretical error in \(H \to Z Z\). More... | |
| double | ettH_1314_DeltagHt |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (13 & 14 TeV). More... | |
| double | ettH_1314_G |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (13 & 14 TeV). More... | |
| double | ettH_1314_HG |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (13 & 14 TeV). More... | |
| double | ettH_1314_uG_33r |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (13 & 14 TeV). More... | |
| double | ettH_2_DeltagHt |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (1.96 TeV). More... | |
| double | ettH_2_G |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (1.96 TeV). More... | |
| double | ettH_2_HG |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (1.96 TeV). More... | |
| double | ettH_2_uG_33r |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (1.96 TeV). More... | |
| double | ettH_78_DeltagHt |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (7 & 8 TeV). More... | |
| double | ettH_78_G |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (7 & 8 TeV). More... | |
| double | ettH_78_HG |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (7 & 8 TeV). More... | |
| double | ettH_78_uG_33r |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (7 & 8 TeV). More... | |
| double | ettHbb |
| double | ettHgaga |
| double | ettHint |
| Intrinsic relative theoretical error in ttH production. (Assumed to be constant in energy.) More... | |
| double | ettHmumu |
| Total relative theoretical error in \(pp \to ttH \to tt X\). More... | |
| double | ettHpar |
| Parametric relative theoretical error in ttH production. (Assumed to be constant in energy.) More... | |
| double | ettHtautau |
| double | ettHWW |
| double | ettHZga |
| double | ettHZZ |
| double | eVBF_1314_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_DHB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_HB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_Hd_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_HG |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_HQ1_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_Hu_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_2_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_DHB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_HB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_Hd_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_HG |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_HQ1_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_Hu_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_78_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_DHB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_HB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_Hd_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_HG |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_HQ1_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_Hu_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBFHbb |
| double | eVBFHgaga |
| double | eVBFHinv |
| double | eVBFHmumu |
| Total relative theoretical error in \(pp \to Hjj (VBF) \to X jj\). More... | |
| double | eVBFHtautau |
| double | eVBFHWW |
| double | eVBFHZga |
| double | eVBFHZZ |
| double | eVBFint |
| Intrinsic relative theoretical error in VBF production. (Assumed to be constant in energy.) More... | |
| double | eVBFpar |
| Parametric relative theoretical error in VBF production. (Assumed to be constant in energy.) More... | |
| double | eVHinv |
| Total relative theoretical error in \(pp \to X H \to X + invisible\). More... | |
| double | eWH_1314_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (13 & 14 TeV). More... | |
| double | eWH_1314_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (13 & 14 TeV). More... | |
| double | eWH_1314_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (13 & 14 TeV). More... | |
| double | eWH_1314_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (13 & 14 TeV). More... | |
| double | eWH_1314_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (13 & 14 TeV). More... | |
| double | eWH_1314_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (13 & 14 TeV). More... | |
| double | eWH_1314_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (13 & 14 TeV). More... | |
| double | eWH_2_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (1.96 TeV). More... | |
| double | eWH_2_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (1.96 TeV). More... | |
| double | eWH_2_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (1.96 TeV). More... | |
| double | eWH_2_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (1.96 TeV). More... | |
| double | eWH_2_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (1.96 TeV). More... | |
| double | eWH_2_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (1.96 TeV). More... | |
| double | eWH_2_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (1.96 TeV). More... | |
| double | eWH_78_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (7 & 8 TeV). More... | |
| double | eWH_78_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (7 & 8 TeV). More... | |
| double | eWH_78_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (7 & 8 TeV). More... | |
| double | eWH_78_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (7 & 8 TeV). More... | |
| double | eWH_78_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (7 & 8 TeV). More... | |
| double | eWH_78_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (7 & 8 TeV). More... | |
| double | eWH_78_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (7 & 8 TeV). More... | |
| double | eWHbb |
| double | eWHgaga |
| double | eWHint |
| Intrinsic relative theoretical error in WH production. (Assumed to be constant in energy.) More... | |
| double | eWHmumu |
| Total relative theoretical error in \(pp \to WH \to W X\). More... | |
| double | eWHpar |
| Parametric relative theoretical error in WH production. (Assumed to be constant in energy.) More... | |
| double | eWHtautau |
| double | eWHWW |
| double | eWHZga |
| double | eWHZZ |
| double | eZH_1314_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_DHB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_HB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_Hd_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_HQ1_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_Hu_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_2_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_DHB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_HB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_Hd_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_HQ1_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_Hu_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_78_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_DHB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_HB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_Hd_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_HQ1_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_Hu_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZHbb |
| double | eZHgaga |
| double | eZHint |
| Intrinsic relative theoretical error in ZH production. (Assumed to be constant in energy.) More... | |
| double | eZHmumu |
| Total relative theoretical error in \(pp \to ZH \to Z X\). More... | |
| double | eZHpar |
| Parametric relative theoretical error in ZH production. (Assumed to be constant in energy.) More... | |
| double | eZHtautau |
| double | eZHWW |
| double | eZHZga |
| double | eZHZZ |
| double | g1_tree |
| The tree level value of the \(U(1)_Y\) gauge coupling contant (at the \(Z\) pole). More... | |
| double | g2_tree |
| The tree level value of the \(SU(2)_L\) gauge coupling contant (at the \(Z\) pole). More... | |
| double | g3_tree |
| The tree level value of the \(SU(3)_c\) gauge coupling contant (at the \(Z\) pole). More... | |
| double | gADdH_11r |
| double | gADdH_22r |
| double | gADdH_33r |
| double | gADDHB |
| double | gADDHW |
| double | gADeH_11r |
| double | gADeH_22r |
| double | gADeH_33r |
| double | gADG |
| double | gADH |
| double | gADHB |
| double | gADHbox |
| double | gADHD |
| double | gADHd_11 |
| double | gADHd_22 |
| double | gADHd_33 |
| double | gADHe_11 |
| double | gADHe_22 |
| double | gADHe_33 |
| double | gADHG |
| double | gADHL1_11 |
| double | gADHL1_22 |
| double | gADHL1_33 |
| double | gADHL3_11 |
| double | gADHL3_22 |
| double | gADHL3_33 |
| double | gADHQ1_11 |
| double | gADHQ1_22 |
| double | gADHQ1_33 |
| double | gADHQ3_11 |
| double | gADHQ3_22 |
| double | gADHQ3_33 |
| double | gADHu_11 |
| double | gADHu_22 |
| double | gADHu_33 |
| double | gADHW |
| double | gADHWB |
| double | gADLL_1221 |
| double | gADuB_11r |
| double | gADuB_22r |
| double | gADuB_33r |
| double | gADuG_11r |
| double | gADuG_22r |
| double | gADuG_33r |
| double | gADuH_11r |
| double | gADuH_22r |
| double | gADuH_33r |
| double | gADuW_11r |
| double | gADuW_22r |
| double | gADuW_33r |
| double | gADW |
| double | GammaHTotR |
| NP contributions and Total to Higgs width ratio with SM. More... | |
| double | gZdL |
| double | gZdR |
| The tree level value of the \(Z\bar{d}d\) couplings in the SM. More... | |
| double | gZlL |
| double | gZlR |
| The tree level value of the \(Z\ell^+\ell^-\) couplings in the SM. More... | |
| double | gZuL |
| double | gZuR |
| The tree level value of the \(Z\bar{u}u\) couplings in the SM. More... | |
| double | gZvL |
| The tree level value of the \(Z\bar{\nu}\nu\) couplings in the SM. More... | |
| double | Lambda_NP |
| The new physics scale [GeV]. More... | |
| double | lambdaH_tree |
| The SM tree level value of the scalar quartic coupling in the potential. More... | |
| double | LambdaNP2 |
| The square of the new physics scale [GeV \(^2\)]. More... | |
| double | lambZ |
| Independent contribution to aTGC. More... | |
| double | Mw_tree |
| The tree level value of the \(W\) boson mass. More... | |
| Matching< NPSMEFTd6Matching, NPSMEFTd6 > | NPSMEFTd6M |
| double | nuisP1 |
| double | nuisP10 |
| Nuisance parameters to be used in observables. More... | |
| double | nuisP2 |
| double | nuisP3 |
| double | nuisP4 |
| double | nuisP5 |
| double | nuisP6 |
| double | nuisP7 |
| double | nuisP8 |
| double | nuisP9 |
| double | sW2_tree |
| The square of the tree level values for the sine of the weak angle. More... | |
| double | sW_tree |
| The tree level values for the sine of the weak angle. More... | |
| double | UevL |
| The tree level value of the \(W^-\bar{\ell}\nu\) couplings in the SM. (Neglecting PMNS effects.) More... | |
| double | v2 |
| The square of the EW vev. More... | |
| double | v2_over_LambdaNP2 |
| The ratio between the EW vev and the new physics scale, squared \(v^2/\Lambda^2\). More... | |
| double | VudL |
| The tree level value of the \(W^+\bar{u}d\) couplings in the SM. (Neglecting CKM effects.) More... | |
| double | xBZ_tree |
| The tree level component of the matrix that transform the gauge field \(B_{\mu}\) into \(Z_{\mu}\). More... | |
| double | xWZ_tree |
| The tree level component of the matrix that transform the gauge field \(W_{\mu}^3\) into \(Z_{\mu}\). More... | |
| double | Yukb |
| SM d-quark Yukawas. More... | |
| double | Yukc |
| double | Yukd |
| double | Yuke |
| double | Yukmu |
| double | Yuks |
| double | Yukt |
| SM u-quark Yukawas. More... | |
| double | Yuktau |
| SM lepton Yukawas. More... | |
| double | Yuku |
| Protected Attributes inherited from NPbase | |
| StandardModel | trueSM |
| Protected Attributes inherited from StandardModel | |
| double | A |
| The CKM parameter \(A\) in the Wolfenstein parameterization. More... | |
| double | ale |
| The fine-structure constant \(\alpha\). More... | |
| double | alpha21 |
| double | alpha31 |
| double | AlsMz |
| The strong coupling constant at the Z-boson mass, \(\alpha_s(M_Z)\). More... | |
| bool | bSigmaForAFB |
| bool | bSigmaForR |
| double | dAl5hMz |
| The five-flavour hadronic contribution to the electromagnetic coupling, \(\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)\). (Non-input parameter) More... | |
| double | dAle5Mz |
| The five-flavour hadronic contribution to the electromagnetic coupling, \(\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)\), used as input for FlagMWinput = FALSE. More... | |
| double | delGammaZ |
| The theoretical uncertainty in \(\Gamma_Z\), denoted as \(\delta\,\Gamma_Z\), in GeV. More... | |
| double | delMw |
| The theoretical uncertainty in \(M_W\), denoted as \(\delta\,M_W\), in GeV. More... | |
| double | delR0b |
| The theoretical uncertainty in \(R_b^0\), denoted as \(\delta\,R_b^0\). More... | |
| double | delR0c |
| The theoretical uncertainty in \(R_c^0\), denoted as \(\delta\,R_c^0\). More... | |
| double | delR0l |
| The theoretical uncertainty in \(R_l^0\), denoted as \(\delta\,R_l^0\). More... | |
| double | delsigma0H |
| The theoretical uncertainty in \(\sigma_{Hadron}^0\), denoted as \(\delta\,\sigma_{Hadron}^0\) in nb. More... | |
| double | delSin2th_b |
| The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{b}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{b}\). More... | |
| double | delSin2th_l |
| The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{\rm lept}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{\rm lept}\). More... | |
| double | delSin2th_q |
| The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{q\not = b,t}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{q\not = b,t}\). More... | |
| double | delta |
| double | etab |
| The CKM parameter \(\bar{\eta}\) in the Wolfenstein parameterization. More... | |
| bool | flag_order [orders_EW_size] |
| An array of internal flags controlling the inclusions of higher-order corrections. More... | |
| bool | FlagFixMuwMut |
| A boolean for the model flag FixMuwMut. More... | |
| bool | flagLEP2 [NUMofLEP2RCs] |
| double | gamma |
| \(\gamma \) used as an input for FlagWolfenstein = FALSE More... | |
| double | GF |
| The Fermi constant \(G_\mu\) in \({\rm GeV}^{-2}\). More... | |
| double | lambda |
| The CKM parameter \(\lambda\) in the Wolfenstein parameterization. More... | |
| Particle | leptons [6] |
| An array of Particle objects for the leptons. More... | |
| double | mHl |
| The Higgs mass \(m_h\) in GeV. More... | |
| double | muw |
| A matching scale \(\mu_W\) around the weak scale in GeV. More... | |
| double | Mw_inp |
| The mass of the \(W\) boson in GeV used as input for FlagMWinput = TRUE. More... | |
| CKM | myCKM |
| An object of type CKM. More... | |
| PMNS | myPMNS |
| double | Mz |
| The mass of the \(Z\) boson in GeV. More... | |
| bool | requireCKM |
| An internal flag to control whether the CKM matrix has to be recomputed. More... | |
| bool | requireYe |
| An internal flag to control whether the charged-lepton Yukawa matrix has to be recomputed. More... | |
| bool | requireYn |
| An internal flag to control whether the neutrino Yukawa matrix has to be recomputed. More... | |
| double | rhob |
| The CKM parameter \(\bar{\rho}\) in the Wolfenstein parameterization. More... | |
| double | s12 |
| double | s13 |
| double | s23 |
| Flavour | SMFlavour |
| An object of type Flavour. More... | |
| Matching< StandardModelMatching, StandardModel > | SMM |
| An object of type Matching. More... | |
| double | Vcb |
| \(\vert V_{cb} \vert \) used as an input for FlagWolfenstein = FALSE More... | |
| double | Vub |
| \(\vert V_{ub} \vert \) used as an input for FlagWolfenstein = FALSE More... | |
| double | Vud |
| \(\vert V_{ud} \vert \) used as an input for FlagWolfenstein = FALSE and FlagUseVud = TRUE More... | |
| double | Vus |
| \(\vert V_{us} \vert \) used as an input for FlagWolfenstein = FALSE More... | |
| gslpp::matrix< gslpp::complex > | Yd |
| The Yukawa matrix of the down-type quarks. More... | |
| gslpp::matrix< gslpp::complex > | Ye |
| The Yukawa matrix of the charged leptons. More... | |
| gslpp::matrix< gslpp::complex > | Yn |
| The Yukawa matrix of the neutrinos. More... | |
| gslpp::matrix< gslpp::complex > | Yu |
| The Yukawa matrix of the up-type quarks. More... | |
| Protected Attributes inherited from QCD | |
| double | AlsM |
| The strong coupling constant at the mass scale MAls, \(\alpha_s(M_{\alpha_s})\). More... | |
| double | CA |
| double | CF |
| bool | computemt |
| Switch for computing the \(\overline{\mathrm{MS}}\) mass of the top quark. More... | |
| double | dAdA_NA |
| double | dFdA_NA |
| double | dFdF_NA |
| bool | FlagMpole2MbarNumeric |
| A flag to determine whether the pole mass to \(\over \mathrm{MS}\) mass conversion is done numerically. More... | |
| bool | FlagMtPole |
| A flag to determine whether the pole mass of the top quark is used as input. More... | |
| double | MAls |
| The mass scale in GeV at which the strong coupling measurement is provided. More... | |
| double | mtpole |
| The pole mass of the top quark. More... | |
| double | mub |
| The threshold between five- and four-flavour theory in GeV. More... | |
| double | muc |
| The threshold between four- and three-flavour theory in GeV. More... | |
| double | mut |
| The threshold between six- and five-flavour theory in GeV. More... | |
| double | NA |
| double | Nc |
| The number of colours. More... | |
| bool | QCDsuccess =true |
| Particle | quarks [6] |
| The vector of all SM quarks. More... | |
| bool | requireYd |
| Switch for generating the Yukawa couplings to the down-type quarks. More... | |
| bool | requireYu |
| Switch for generating the Yukawa couplings to the up-type quarks. More... | |
| double | TF |
| Protected Attributes inherited from Model | |
| bool | isSliced = false |
| A boolean set to true if the current istance is a slice of an extended object. More... | |
| std::map< std::string, std::reference_wrapper< const double > > | ModelParamMap |
| bool | UpdateError = false |
| A boolean set to false if update is successful. More... | |
Private Attributes | |
| bool | FlagFlavU3OfX |
| A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients. More... | |
| bool | FlagHiggsSM |
| A boolean flag that is true if including dependence on small variations of the SM parameters (dependence is linearized). Available only in selected Higgs observables. More... | |
| const bool | FlagLeptonUniversal |
| An internal boolean flag that is true if assuming lepton flavour universality. More... | |
| bool | FlagLoopH3d6Quad |
| A boolean flag that is true if including quadratic modifications in the SM loops in Higgs observables due to the dim 6 interactions that contribute to the trilinear Higgs coupling. More... | |
| bool | FlagLoopHd6 |
| A boolean flag that is true if including modifications in the SM loops in Higgs observables due to the dim 6 interactions. More... | |
| bool | FlagMWinput |
| A boolean for the model flag MWinput. More... | |
| bool | FlagPartialQFU |
| A boolean flag that is true if assuming partial quark flavour universality between the 1st and 2nd family in the CHF operators. More... | |
| bool | FlagQuadraticTerms |
| A boolean flag that is true if the quadratic terms in cross sections and widths are switched on. More... | |
| const bool | FlagQuarkUniversal |
| An internal boolean flag that is true if assuming quark flavour universality. More... | |
| bool | FlagRGEciLLA |
| A flag that is TRUE if including log-enhanced 1-loop corrections propotional to the dim-6 Wilson coefficients. See comment in documentation above. More... | |
| bool | FlagRotateCHWCHB |
| A boolean flag that is true if we use as parameters CHWHB_gaga and CHWHB_gagaorth instead of CHW and CHB. More... | |
| bool | FlagUnivOfX |
| A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients and all proportional to the same coefficient (CuH_33 and CuV_33 respectively). More... | |
| gsl_integration_cquad_workspace * | w_WW |
Additional Inherited Members | |
| Public Types inherited from StandardModel | |
| enum | LEP2RCs { Weak = 0 , WeakBox , ISR , QEDFSR , QCDFSR , NUMofLEP2RCs } |
| enum | orders_EW { EW1 = 0 , EW1QCD1 , EW1QCD2 , EW2 , EW2QCD1 , EW3 , orders_EW_size } |
| An enumerated type representing perturbative orders of radiative corrections to EW precision observables. More... | |
| Public Types inherited from QCD | |
| enum | lepton { NEUTRINO_1 , ELECTRON , NEUTRINO_2 , MU , NEUTRINO_3 , TAU , NOLEPTON } |
| An enum type for leptons. More... | |
| enum | meson { P_0 , P_P , K_0 , K_P , D_0 , D_P , D_S , B_D , B_P , B_S , B_C , PHI , K_star , K_star_P , K_S , D_star_P , RHO , RHO_P , OMEGA , MESON_END } |
| An enum type for mesons. More... | |
| enum | quark { UP , DOWN , CHARM , STRANGE , TOP , BOTTOM } |
| An enum type for quarks. More... | |
| Public Attributes inherited from NPbase | |
| double | C1Hbb = 0.0 |
| double | C1Hcc = 0.0 |
| double | C1Hgaga = 0.0049 |
| double | C1Hgg = 0.0066 |
| double | C1Hmumu = 0.0 |
| The C1 coefficient controlling the H^3 corrections to the Higgs partial width from the Higgs trilinear coupling. More... | |
| double | C1Hss = 0.0 |
| double | C1Htautau = 0.0 |
| double | C1HWW = 0.0073 |
| double | C1HZga = 0.0 |
| The C1 coefficient controlling the H^3 corrections to the Higgs partial width from the Higgs trilinear coupling. More... | |
| double | C1HZZ = 0.0083 |
| NPSMEFTd6::NPSMEFTd6 | ( | const bool | FlagLeptonUniversal_in = false, |
| const bool | FlagQuarkUniversal_in = false |
||
| ) |
Constructor.
| [in] | FlagLeptonUniversal_in | an internal boolean flag that is true if assuming lepton flavour universality |
| [in] | FlagQuarkUniversal_in | an internal boolean flag that is true if assuming quark flavour universality |
Definition at line 347 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::AH_f | ( | double | tau | ) | const |
Fermionic loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings.
\(A^H_f(\tau)=2\tau [1+(1-\tau)f(\tau)]\)
| [in] |
_form#4670, with \(M\) the mass of the fermion in the loop.
Definition at line 5113 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::AH_W | ( | double | tau | ) | const |
W loop function entering in the calculation of the effective \(H\gamma\gamma\) coupling.
\(A^H_W(\tau)=-[2+3\tau + 3\tau*(2-\tau) f(\tau)]\)
| [in] |
_form#4670, with \(M\) the mass of the fermion in the loop.
Definition at line 5118 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::AHZga_f | ( | double | tau, |
| double | lambda | ||
| ) | const |
Fermionic loop function entering in the calculation of the effective \(HZ\gamma\) coupling.
| [in] |
_form#4670, \(\lambda=4 M^2/m_Z^2\), with \(M\) the mass of the fermion in the loop.
Definition at line 5123 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::AHZga_W | ( | double | tau, |
| double | lambda | ||
| ) | const |
W loop function entering in the calculation of the effective \(HZ\gamma\) coupling.
| [in] |
_form#4670, \(\lambda=4 M^2/m_Z^2\), with \(M\) the mass of the fermion in the loop.
Definition at line 5128 of file NPSMEFTd6.cpp.
|
virtual |
The electromagnetic coupling at the \(Z\)-mass scale.
\(\newcommand{\nc}{\newcommand}\) \(\nc{\gwt}{\widetilde{g}_W}\) \(\nc{\gbt}{\widetilde{g}_1}\) \(\nc{\gbL}{\Delta g_1^{(1)}}\) \(\nc{\gwL}{\Delta g_W^{(1)}}\) \(\nc{\gbQ}{\Delta g_1^{(2)}}\) \(\nc{\gwQ}{\Delta g_W^{(2)}}\) \(\nc{\vt}{\widetilde{v}}\) \(\nc{\dGf}{\delta_{G_F}}\) \(\nc{\swt}{s_W}\) \(\nc{\cwt}{c_W}\)
\[ \alpha (M_Z) = \alpha (M_Z)^{SM} + \Delta \alpha (Mz)^{(1)} + \Delta \alpha (Mz)^{(2)} \]
where,
\[ \Delta \alpha^{(1)} = 2\swt^2\frac{\gwL}{\gwt} + 2\cwt^2\frac{\gbL}{\gbt} - 4\swt\cwt C_{\varphi WB}\frac{\vt^2}{\Lambda^2} \]
\begin{eqnarray*} \Delta \alpha^{(2)} &=& 2\swt^2\frac{\gwQ}{\gwt} + 2\cwt^2\frac{\gbQ}{\gbt} + \swt^2(\swt^2-3\cwt^2)\left(\frac{\gwL}{\gwt}\right)^2 + \cwt^2(\cwt^2-3\swt^2)\left(\frac{\gbL}{\gbt}\right)^2 + 8 \swt^2\cwt^2 \frac{\gwL}{\gwt}\frac{\gbL}{\gbt} \\ &+& 2 \swt\cwt\left((\cwt^2-3\swt^2)\frac{\gwL}{\gwt} + (\swt^2-3\cwt^2)\frac{\gbL}{\gbt}\right) \hat{C}_{\varphi WB} \vt^2 - 2 \swt \cwt \left( -2\swt\cwt \hat{C}_{\varphi WB}\vt^2 + (\hat{C}_{\varphi W}+\hat{C}_{\varphi B})\vt^2 + \dGf^{(1)} \right) \hat{C}_{\varphi WB}\vt^2 \end{eqnarray*}
Reimplemented from NPbase.
Definition at line 4130 of file NPSMEFTd6.cpp.
|
virtual |
the angular parameter \(a\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]).
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 10729 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP1 (See code for details.)
Reimplemented from NPbase.
Definition at line 24249 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP10 (See code for details.)
Reimplemented from NPbase.
Definition at line 24850 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP11 (See code for details.)
Reimplemented from NPbase.
Definition at line 24881 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP12 (See code for details.)
Reimplemented from NPbase.
Definition at line 24912 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP13.
Reimplemented from NPbase.
Definition at line 24928 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP14.
Reimplemented from NPbase.
Definition at line 24944 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP15.
Reimplemented from NPbase.
Definition at line 25056 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP16.
Reimplemented from NPbase.
Definition at line 25275 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP17.
Reimplemented from NPbase.
Definition at line 25494 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP18.
Reimplemented from NPbase.
Definition at line 25514 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP19.
Reimplemented from NPbase.
Definition at line 25534 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP2 (See code for details.)
Reimplemented from NPbase.
Definition at line 24276 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP20.
Reimplemented from NPbase.
Definition at line 25562 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP21 (See code for details.)
Reimplemented from NPbase.
Definition at line 25592 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP22 (See code for details.)
Reimplemented from NPbase.
Definition at line 25637 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP23.
Reimplemented from NPbase.
Definition at line 25691 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP24.
Reimplemented from NPbase.
Definition at line 25727 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP25.
Reimplemented from NPbase.
Definition at line 25772 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP26.
Reimplemented from NPbase.
Definition at line 25779 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP27.
Reimplemented from NPbase.
Definition at line 25786 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP28.
Reimplemented from NPbase.
Definition at line 25793 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP29.
Reimplemented from NPbase.
Definition at line 25800 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP3 (See code for details.)
Reimplemented from NPbase.
Definition at line 24304 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP30.
Reimplemented from NPbase.
Definition at line 25807 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP4 (See code for details.)
Reimplemented from NPbase.
Definition at line 24332 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP5 (See code for details.)
Reimplemented from NPbase.
Definition at line 24396 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP6 (See code for details.)
Reimplemented from NPbase.
Definition at line 24467 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP7 (See code for details.)
Reimplemented from NPbase.
Definition at line 24735 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP8 (See code for details.)
Reimplemented from NPbase.
Definition at line 24768 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP9 (See code for details.)
Reimplemented from NPbase.
Definition at line 24788 of file NPSMEFTd6.cpp.
|
virtual |
the angular parameter \(b\) from \(\mu_{e^+e^- \to ZH}\) (arXiv:1708.09079 [hep-ph]).
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 10812 of file NPSMEFTd6.cpp.
|
virtual |
The branching ratio of the of the Higgs into exotic particles.
Reimplemented from NPbase.
Definition at line 17153 of file NPSMEFTd6.cpp.
|
virtual |
The branching ratio of the of the Higgs into invisible particles.
Reimplemented from NPbase.
Definition at line 17160 of file NPSMEFTd6.cpp.
|
virtual |
The branching ratio of the of the Higgs into invisible particles (only invisible new particles).
Reimplemented from NPbase.
Definition at line 17174 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 2d2d)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 14495 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 2e 2\mu)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 13814 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 2e2v)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 14206 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 2ev)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 16461 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 14804 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 13718 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 14700 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 14110 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 14010 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 16791 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 16363 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 16261 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 2\mu 2v)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 14301 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 2ev)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 16559 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 2u2d)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 14598 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 2u2u)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 14397 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 2ud)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 16156 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 2v2d)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 15004 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 2v2u)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 14903 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 2v2v)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 13909 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 4d)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 15675 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 4e)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 15291 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 4f)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 16660 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 15198 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 15102 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 16725 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 4\mu)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 15384 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 4u)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 15576 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to 4v)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 15479 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to b\bar{b})\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 13620 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to c\bar{c})\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 13523 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to e\nu \mu\nu)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 15862 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to \gamma\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 13277 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to gg)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 12701 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to l l \nu\nu, l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 17125 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to l \nu l \nu, l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 17059 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 16992 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 16051 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 15769 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to \mu^+\mu^-)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 13354 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to \tau^+\tau^-)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 13432 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to invisible)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 17230 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to uddu)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 15955 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to visible)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 17183 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to VV)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 13039 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 12851 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to WW)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 12775 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to Z\gamma\to ee\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 13171 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to Z\gamma\to ll\gamma)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 13156 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to Z\gamma\to \mu\mu\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 13182 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to Z\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 13130 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 13014 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 12924 of file NPSMEFTd6.cpp.
The branching ratio of the \(W\) boson decaying into a SM fermion pair, \(Br(W\to f_i f_j)\).
\[ BrW_{fi,fj} = BrW_{fi,fj}^{SM} + \Delta BrW_{fi,fj}^{(1)} + \Delta BrW_{fi,fj}^{(2)} \]
where,
\[ \Delta BrW_{fi,fj}^{(1)} = \frac{\Gamma_{W, f_i f_j}^{SM}}{\Gamma_W^{SM}} \left( \frac{\Delta \Gamma_{W, f_i f_j}^{(1)}}{\Gamma_{W, f_i f_j}^{SM}} - \frac{\Delta \Gamma_{W}^{(1)}}{\Gamma_{W}^{SM}} \right) \]
\[ \Delta BrW_{fi,fj}^{(2)} = \frac{\Gamma_{W,f_i f_j}^{SM}}{\Gamma_W^{SM}} \left( \frac{\Delta \Gamma_{W, f_i f_j}^{(2)}}{\Gamma_{W, f_i f_j}^{SM}} - \frac{\Delta \Gamma_{W}^{(2)}}{\Gamma_{W}^{SM}} + \frac{(\Delta \Gamma_{W}^{(1)})^2}{(\Gamma_{W}^{SM})^2} + \frac{\Delta \Gamma_{W,f_i f_j}^{(1)} \Delta \Gamma_{W}^{(1)}}{\Gamma_{W, f_i f_j}^{SM} \Gamma_{W}^{SM}} \right) \]
Reimplemented from NPbase.
Definition at line 4568 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeLL_bottom | ( | ) | const |
Definition at line 25857 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeLL_charm | ( | ) | const |
Definition at line 25837 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeLL_down | ( | ) | const |
Definition at line 25847 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeLL_e | ( | ) | const |
Definition at line 25818 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeLL_mu | ( | ) | const |
Definition at line 25822 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeLL_strange | ( | ) | const |
Definition at line 25852 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeLL_tau | ( | ) | const |
Definition at line 25827 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeLL_top | ( | ) | const |
Definition at line 25842 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeLL_up | ( | ) | const |
Definition at line 25832 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeLR_bottom | ( | ) | const |
Definition at line 25901 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeLR_charm | ( | ) | const |
Definition at line 25881 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeLR_down | ( | ) | const |
Definition at line 25891 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeLR_e | ( | ) | const |
Definition at line 25862 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeLR_mu | ( | ) | const |
Definition at line 25866 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeLR_strange | ( | ) | const |
Definition at line 25896 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeLR_tau | ( | ) | const |
Definition at line 25871 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeLR_top | ( | ) | const |
Definition at line 25886 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeLR_up | ( | ) | const |
Definition at line 25876 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeRL_bottom | ( | ) | const |
Definition at line 25946 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeRL_charm | ( | ) | const |
Definition at line 25926 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeRL_down | ( | ) | const |
Definition at line 25936 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeRL_e | ( | ) | const |
Definition at line 25906 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeRL_mu | ( | ) | const |
Definition at line 25911 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeRL_strange | ( | ) | const |
Definition at line 25941 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeRL_tau | ( | ) | const |
Definition at line 25916 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeRL_top | ( | ) | const |
Definition at line 25931 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeRL_up | ( | ) | const |
Definition at line 25921 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeRR_bottom | ( | ) | const |
Definition at line 25990 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeRR_charm | ( | ) | const |
Definition at line 25970 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeRR_down | ( | ) | const |
Definition at line 25980 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeRR_e | ( | ) | const |
Definition at line 25951 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeRR_mu | ( | ) | const |
Definition at line 25955 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeRR_strange | ( | ) | const |
Definition at line 25985 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeRR_tau | ( | ) | const |
Definition at line 25960 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeRR_top | ( | ) | const |
Definition at line 25975 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::CeeRR_up | ( | ) | const |
Definition at line 25965 of file NPSMEFTd6.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{11}\).
Reimplemented from NPbase.
Definition at line 23915 of file NPSMEFTd6.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{22}\).
Reimplemented from NPbase.
Definition at line 23920 of file NPSMEFTd6.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hd})_{33}\).
Reimplemented from NPbase.
Definition at line 23925 of file NPSMEFTd6.cpp.
|
virtual |
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{He})_{22}\).
Reimplemented from NPbase.
Definition at line 23890 of file NPSMEFTd6.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{He})_{33}\).
Reimplemented from NPbase.
Definition at line 23895 of file NPSMEFTd6.cpp.
|
virtual |
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(1)})_{22}\).
Reimplemented from NPbase.
Definition at line 23824 of file NPSMEFTd6.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(1)})_{33}\).
Reimplemented from NPbase.
Definition at line 23829 of file NPSMEFTd6.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(3)})_{11}\).
Reimplemented from NPbase.
Definition at line 23834 of file NPSMEFTd6.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(3)})_{22}\).
Reimplemented from NPbase.
Definition at line 23839 of file NPSMEFTd6.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HL}^{(3)})_{33}\).
Reimplemented from NPbase.
Definition at line 23844 of file NPSMEFTd6.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{11}\).
Reimplemented from NPbase.
Definition at line 23849 of file NPSMEFTd6.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(1)})_{22}\).
Reimplemented from NPbase.
Definition at line 23854 of file NPSMEFTd6.cpp.
|
virtual |
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{11}\).
Reimplemented from NPbase.
Definition at line 23864 of file NPSMEFTd6.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{22}\).
Reimplemented from NPbase.
Definition at line 23869 of file NPSMEFTd6.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(3)})_{33}\).
Reimplemented from NPbase.
Definition at line 23874 of file NPSMEFTd6.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{HQ}^{(d)})_{33}\).
Reimplemented from NPbase.
Definition at line 23879 of file NPSMEFTd6.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{11}\).
Reimplemented from NPbase.
Definition at line 23900 of file NPSMEFTd6.cpp.
|
virtual |
Combination of coefficients of the Warsaw basis constrained by EWPO \((\hat{C}_{Hu})_{22}\).
Reimplemented from NPbase.
Definition at line 23905 of file NPSMEFTd6.cpp.
|
virtual |
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{EB,UB,DB}\) corresponding to particle f.
| [in] | f | a lepton or quark |
Definition at line 3884 of file NPSMEFTd6.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{UG,DG}\) corresponding to particle f.
| [in] | f | a lepton or quark |
Definition at line 3832 of file NPSMEFTd6.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{EH,UH,DH}\) corresponding to particle f.
| [in] | f | a lepton or quark |
Definition at line 3806 of file NPSMEFTd6.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{EW,UW,DW}\) corresponding to particle f.
| [in] | f | a lepton or quark |
Definition at line 3858 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(c_{\gamma\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 23772 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(c_{gg}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 23781 of file NPSMEFTd6.cpp.
|
virtual |
The effective Higgs-basis coupling \(c_{gg}^{Eff}\). (Similar to cgg_HB but including modifications of SM loops.) (See arXiv: 1505.00046 [hep-ph] document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 23790 of file NPSMEFTd6.cpp.
|
virtual |
A method to check if all the mandatory parameters for NPSMEFTd6 have been provided in model initialization.
| [in] | DPars | a map of the parameters that are being updated in the Monte Carlo run (including parameters that are varied and those that are held constant) |
Reimplemented from StandardModel.
Definition at line 3040 of file NPSMEFTd6.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(1)}\) corresponding to particle F.
| [in] | F | a lepton or quark |
Definition at line 3729 of file NPSMEFTd6.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(3)}\) corresponding to particle F.
| [in] | F | a lepton or quark |
Definition at line 3747 of file NPSMEFTd6.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{HE,HU,HD}\) corresponding to particle f.
| [in] | f | a lepton or quark |
Definition at line 3765 of file NPSMEFTd6.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{Hud}\) corresponding to particle f.
| [in] | u | a quark |
Definition at line 3791 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 12547 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(c_{z\Box}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 23739 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(c_{z\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 23761 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(c_{zz}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 23750 of file NPSMEFTd6.cpp.
|
virtual |
Quadratic contribution from the Higgs self-couplings modifications to the signal strength for \(\sigma \times BR(H\to xx)\) in the current model.
Reimplemented from NPbase.
Definition at line 3951 of file NPSMEFTd6.cpp.
|
virtual |
Quadratic contribution from the Higgs self-couplings modifications to the signal strength for an observable \(\sigma\) in the current model.
Reimplemented from NPbase.
Definition at line 3939 of file NPSMEFTd6.cpp.
|
virtual |
Reimplemented from NPbase.
Definition at line 26902 of file NPSMEFTd6.cpp.
|
virtual |
Reimplemented from NPbase.
Definition at line 26494 of file NPSMEFTd6.cpp.
|
virtual |
Reimplemented from NPbase.
Definition at line 26416 of file NPSMEFTd6.cpp.
|
inlinevirtual |
The SMEFT linear correction to the ratio \(\mu_{bbH}\) between the bbH production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 2542 of file NPSMEFTd6.h.
|
inlinevirtual |
The SMEFT quadratic correction to the ratio \(\mu_{bbH}\) between the bbH production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 2546 of file NPSMEFTd6.h.
|
virtual |
The SMEFT linear correction to the ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 5141 of file NPSMEFTd6.cpp.
|
inlinevirtual |
The SMEFT quadratic correction to the ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 2497 of file NPSMEFTd6.h.
|
inlinevirtual |
The SMEFT linear correction to the ratio \(\mu_{tH}\) between the t-Higgs associated production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 2532 of file NPSMEFTd6.h.
|
inlinevirtual |
The SMEFT quadratic correction to the ratio \(\mu_{tH}\) between the t-Higgs associated production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 2537 of file NPSMEFTd6.h.
|
virtual |
The SMEFT linear correction to the ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 10895 of file NPSMEFTd6.cpp.
|
inlinevirtual |
The SMEFT quadratic correction to the ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 2527 of file NPSMEFTd6.h.
|
virtual |
The SMEFT linear correction to the ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 5294 of file NPSMEFTd6.cpp.
|
inlinevirtual |
The SMEFT quadratic correction to the ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 2503 of file NPSMEFTd6.h.
|
virtual |
The SMEFT linear correction to the ratio \(\mu_{VH}\) between the Z-Higgs and W-Higgs associated production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 10840 of file NPSMEFTd6.cpp.
|
inlinevirtual |
The SMEFT quadratic correction to the ratio \(\mu_{VH}\) between the Z-Higgs and W-Higgs associated production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 2521 of file NPSMEFTd6.h.
|
virtual |
The SMEFT linear correction to the ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 8785 of file NPSMEFTd6.cpp.
|
inlinevirtual |
The SMEFT quadratic correction to the ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 2509 of file NPSMEFTd6.h.
|
virtual |
The SMEFT linear correction to the ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 9033 of file NPSMEFTd6.cpp.
|
inlinevirtual |
The SMEFT quadratic correction to the ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 2515 of file NPSMEFTd6.h.
|
virtual |
Reimplemented from NPbase.
Definition at line 26866 of file NPSMEFTd6.cpp.
|
virtual |
Reimplemented from NPbase.
Definition at line 26453 of file NPSMEFTd6.cpp.
|
virtual |
Reimplemented from NPbase.
Definition at line 26480 of file NPSMEFTd6.cpp.
|
virtual |
|
virtual |
Reimplemented from NPbase.
Definition at line 26490 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the electromagnetic constant at zero momentum, \(\delta \alpha(0)/\alpha(0)\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 4093 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the electromagnetic constant at zero momentum, \((\delta \alpha(0)/\alpha(0))^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 4099 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the electromagnetic constant at the Z pole, \(\delta \alpha(M_Z^2)/\alpha(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 4082 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the electromagnetic constant at the Z pole, \((\delta \alpha(M_Z^2)/\alpha(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 4088 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the strong coupling constant at the Z pole, \(\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 4104 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the strong coupling constant at the Z pole, \((\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 4110 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(\delta c_z\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 23730 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the differential cross section in pb for \(e^+ e^- \to W^+ W^- \to lv jj \), with \( l= e,\mu \) for the 4 \( cos{\theta}\) bins defined in arXiv: 1606.06693 [hep-ph]. for the C.O.M. energies of 182.6 and 205.9 GeV. From arXiv: 1606.06693 [hep-ph].
Reimplemented from NPbase.
Definition at line 19511 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 4771 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 4814 of file NPSMEFTd6.cpp.
|
virtual |
The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.
Reimplemented from NPbase.
Definition at line 4819 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 4795 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the anomalous triple gauge coupling \(g_{1,\gamma}\).
Reimplemented from NPbase.
Definition at line 18334 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the anomalous triple gauge coupling \(g_{1,Z}\).
Reimplemented from NPbase.
Definition at line 18309 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the effective anomalous triple gauge coupling \(g_{1,Z}^{Eff}\) from arXiv: 1708.09079 [hep-ph].
Reimplemented from NPbase.
Definition at line 18370 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 4776 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 4899 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 4800 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\).
Reimplemented from NPbase.
Definition at line 4781 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\).
Reimplemented from NPbase.
Definition at line 4805 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltag3G | ( | ) | const |
The new physics contribution to the coupling of the effective interaction \(f_{ABC} G_{\mu\nu}^A G_{\nu\rho}^B G_{\rho\mu}^C\).
Definition at line 5059 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::deltaG_Aff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 5052 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::deltaG_Gff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 5038 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 4904 of file NPSMEFTd6.cpp.
|
virtual |
The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.
Reimplemented from NPbase.
Definition at line 4909 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::deltaG_hAff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(H A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 5031 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\).
| [in] | p | a lepton or quark |
Reimplemented from NPbase.
Definition at line 4962 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::deltaG_hGff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 5017 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\).
Reimplemented from NPbase.
Definition at line 4744 of file NPSMEFTd6.cpp.
|
virtual |
The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.
Reimplemented from NPbase.
Definition at line 4749 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value.
Reimplemented from NPbase.
Definition at line 4976 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::deltaG_hZff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 5024 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::deltaG_Zff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 5045 of file NPSMEFTd6.cpp.
|
virtual |
New physics contribution to the neutral-current axial-vector coupling \(g_A^f\).
| [in] | f | a lepton or quark |
Reimplemented from NPbase.
Definition at line 4427 of file NPSMEFTd6.cpp.
|
virtual |
The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the neutral-current vector coupling \(g_A^f\).
\[ \Delta g_{A,f}^{(2)} = \Delta g_{L,f}^{(2)} - \Delta g_{R,f}^{(2)} \]
| [in] | f | a lepton or quark |
Reimplemented from NPbase.
Definition at line 4440 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the total decay width of the \(W\) boson, \(\delta \Gamma_W\).
Reimplemented from NPbase.
Definition at line 4342 of file NPSMEFTd6.cpp.
|
virtual |
Definition at line 4312 of file NPSMEFTd6.cpp.
The new physics contribution to the decay width of the \(W\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\).
| [in] | fi | a lepton or quark |
| [in] | fj | a lepton or quark |
Reimplemented from NPbase.
Definition at line 4260 of file NPSMEFTd6.cpp.
Definition at line 4223 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2d2dRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2d2d)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 14438 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2d2dRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2d2d)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 14486 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2e2muRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2e 2\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 13759 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2e2muRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2e 2\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 13805 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2e2vRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2e2v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 14151 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2e2vRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2e2v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 14197 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2evRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2ev)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 16404 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2evRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2ev)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 16452 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2L2dRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 14741 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2L2dRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 14795 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2L2LRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 13661 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2L2LRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 13709 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2L2uRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 14639 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2L2uRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 14691 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2L2v2Ratio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 14051 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2L2v2Ratio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 14101 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2L2vRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 13950 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2l2vRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 16766 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2L2vRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 14001 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2l2vRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 16782 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2Lv2Ratio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 16302 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2Lv2Ratio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 16354 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2LvRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 16197 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2LvRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 16252 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2mu2vRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2\mu 2v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 14247 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2mu2vRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2\mu 2v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 14292 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2muvRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2\mu v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 16502 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2muvRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2\mu v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 16550 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2u2dRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2u2d)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 14536 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2u2dRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2u2d)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 14589 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2u2uRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2u2u)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 14342 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2u2uRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2u2u)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 14388 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2udRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2ud)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 16092 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2udRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2ud)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 16147 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2v2dRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2v2d)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 14944 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2v2dRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2v2d)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 14995 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2v2uRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2v2u)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 14845 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2v2uRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2v2u)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 14894 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2v2vRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2v2v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 13855 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH2v2vRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 2v2v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 13900 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH4dRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4d)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 15617 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH4dRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4d)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 15666 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH4eRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4e)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 15239 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH4eRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4e)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 15282 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH4fRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4f)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 16600 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH4fRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4f)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 16629 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH4L2Ratio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 15143 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH4L2Ratio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 15189 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH4LRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 15045 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH4lRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 16701 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH4LRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 15093 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH4lRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 16716 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH4muRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 15332 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH4muRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 15375 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH4uRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4u)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 15520 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH4uRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4u)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 15567 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH4vRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4v)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 15425 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaH4vRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to 4v)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 15470 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 13564 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 13610 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 13474 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 13513 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaHevmuvRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to e\nu \mu\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 15810 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaHevmuvRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to e\nu \mu\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 15853 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 13209 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 13267 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients.
Reimplemented from NPbase.
Definition at line 12648 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 12691 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaHll_vvorjjRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to l l \nu\nu, l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 17100 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaHll_vvorjjRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to l l \nu\nu, l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 17116 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaHlv_lvorjjRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to l \nu l \nu, l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 17033 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaHlv_lvorjjRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to l \nu l \nu, l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 17050 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaHlvjjRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 16938 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaHlvjjRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 16983 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaHLvudRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 15996 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaHLvudRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 16042 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaHLvvLRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 15716 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaHLvvLRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 15760 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 13319 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 13344 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 13396 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 13422 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaHudduRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to uddu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 15903 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaHudduRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to uddu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 15946 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaHWW4fRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 12798 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaHWW4fRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 12841 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 12743 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 12763 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 13062 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 13120 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaHZZ4fRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 12945 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGammaHZZ4fRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 13004 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 12892 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Reimplemented from NPbase.
Definition at line 12912 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients.
Reimplemented from NPbase.
Definition at line 12564 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. Neglecting SM theory errors.
Definition at line 12587 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are quadratic in the effective Lagrangian coefficients.
Reimplemented from NPbase.
Definition at line 12612 of file NPSMEFTd6.cpp.
|
virtual |
New physics contribution to the Fermi constant.
The new physics contribution \(\Delta G\) is defined as
\[ G_\mu = G_{\mu,\mathrm{SM}}(1+\Delta G)\,, \]
where \(G_\mu\) is the experimental value measured through muon decays, and \(G_{\mu,\mathrm{SM}}\) is the Fermi constant in the SM.
Reimplemented from NPbase.
Definition at line 3968 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGL_f | ( | const Particle | p | ) | const |
New physics contribution to the neutral-current left-handed coupling \(g_L^f\).
| [in] | f | a lepton or quark |
Definition at line 4453 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGL_f_2 | ( | const Particle | p | ) | const |
The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the left-handed coupling \(g_L^f\).
\(\newcommand{\nc}{\newcommand}\) \(\nc{\vt}{\widetilde{v}}\) \(\nc{\xWZb}{\mathbb{\bar{X}}_{(WZ)}}\) \(\nc{\xBZb}{\mathbb{\bar{X}}_{(BZ)}}\) \(\nc{\xWZt}{\mathbb{\widetilde{X}}_{(WZ)}}\) \(\nc{\xBZt}{\mathbb{\widetilde{X}}_{(BZ)}}\) \(\nc{\xWZL}{\Delta \mathbb{X}_{WZ}^{(1)}}\) \(\nc{\xBZL}{\Delta \mathbb{X}_{BZ}^{(1)}}\) \(\nc{\xWZQ}{\Delta \mathbb{X}_{WZ}^{(2)}}\) \(\nc{\xBZQ}{\Delta \mathbb{X}_{BZ}^{(2)}}\) \(\nc{\gwt}{\widetilde{g}_W}\) \(\nc{\gbt}{\widetilde{g}_1}\) \(\nc{\gbL}{\Delta g_1^{(1)}}\) \(\nc{\gwL}{\Delta g_W^{(1)}}\) \(\nc{\gbQ}{\Delta g_1^{(2)}}\) \(\nc{\gwQ}{\Delta g_W^{(2)}}\)
\begin{eqnarray*} \Delta g_L^{(2)} &=& \frac{1}{\sqrt{\gbt^2+\gwt^2}} \left[ (Q-I_3) ~\left(\gbt ~\xBZQ + \gbL \xBZL + \xBZt \gbQ \right) + I_3 ~\left(\gwt \xWZQ + \gwL \xWZL + \xWZt \gwQ \right) \right] \\ &+& \frac{(\hat{C}_{Hf1} - 2I_3\hat{C}_{Hf3}) \vt^2}{2} ~\frac{\xBZt \gbL + \gbt \xBZL - \xWZt \gwL - \gwt \xWZL }{\sqrt{\gbt^2+\gwt^2}} \end{eqnarray*}
| [in] | f | a lepton or quark |
Definition at line 4470 of file NPSMEFTd6.cpp.
New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\).
| [in] | pbar | a lepton or quark |
| [in] | p | a lepton or quark |
Reimplemented from NPbase.
Definition at line 4718 of file NPSMEFTd6.cpp.
The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_L}\gamma^mu f_L\).
| [in] | pbar | a lepton or quark |
| [in] | p | a lepton or quark |
Definition at line 4985 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGL_Zffh | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_L}\gamma^mu f_L\).
| [in] | p | a lepton or quark |
Definition at line 5003 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the muon decay constant, \(\delta G_\mu/G_\mu\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 4071 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the muon decay constant, \((\delta G_\mu/G_\mu)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 4077 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGR_f | ( | const Particle | p | ) | const |
New physics contribution to the neutral-current right-handed coupling \(g_R^f\).
| [in] | f | a lepton or quark |
Definition at line 4512 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGR_f_2 | ( | const Particle | p | ) | const |
The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the right-handed coupling \(g_R^f\).
\[ \Delta g_R^{(2)} = \frac{Q}{\sqrt{\gbt^2+\gwt^2}} \left( \gbt \xBZQ + \gbL \xBZL + \xBZt \gbQ \right) + \frac{\hat{C}_{Hf} \vt^2}{2} ~\frac{\xBZt \gbL + \gbt \xBZL - \xWZt \gwL - \gwt \xWZL }{\sqrt{\gbt^2+\gwt^2}} \]
| [in] | f | a lepton or quark |
Definition at line 4527 of file NPSMEFTd6.cpp.
New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\).
| [in] | pbar | a lepton or quark |
| [in] | p | a lepton or quark |
Reimplemented from NPbase.
Definition at line 4735 of file NPSMEFTd6.cpp.
The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_R}\gamma^mu f_R\).
| [in] | pbar | a lepton or quark |
| [in] | p | a lepton or quark |
Definition at line 4994 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaGR_Zffh | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_R}\gamma^mu f_R\).
| [in] | p | a lepton or quark |
Definition at line 5011 of file NPSMEFTd6.cpp.
|
virtual |
New physics contribution to the neutral-current vector coupling \(g_V^f\).
| [in] | f | a lepton or quark |
Reimplemented from NPbase.
Definition at line 4401 of file NPSMEFTd6.cpp.
|
virtual |
The \(\mathcal{O}(\Lambda^{-4})\) new physics contribution to the neutral-current vector coupling \(g_V^f\).
\[ \Delta g_{V,f}^{(2)} = \Delta g_{L,f}^{(2)} + \Delta g_{R,f}^{(2)} \]
| [in] | f | a lepton or quark |
Reimplemented from NPbase.
Definition at line 4414 of file NPSMEFTd6.cpp.
|
virtual |
The relative NP corrections to the width of the \(W\) boson, \(\delta \Gamma_W/\Gamma_W\).
Definition at line 4377 of file NPSMEFTd6.cpp.
|
virtual |
The relative NP corrections to the width of the \(W\) boson squared, \((\delta \Gamma_W/\Gamma_W)^2\).
Definition at line 4382 of file NPSMEFTd6.cpp.
|
virtual |
The relative NP corrections to the width of the \(Z\) boson, \(\delta \Gamma_Z/\Gamma_Z\).
Definition at line 4389 of file NPSMEFTd6.cpp.
|
virtual |
The relative NP corrections to the width of the \(Z\) boson squared, \((\delta \Gamma_Z/\Gamma_Z)^2\).
Definition at line 4394 of file NPSMEFTd6.cpp.
|
virtual |
The coefficient of the 1-loop linear term in the Higgs selfcoupling.
Definition at line 3916 of file NPSMEFTd6.cpp.
|
virtual |
|
virtual |
The new physics contribution to the anomalous triple gauge coupling \(\kappa_{\gamma}\).
Reimplemented from NPbase.
Definition at line 18343 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the effective anomalous triple gauge coupling \(\kappa_{\gamma}^{Eff}\) from arXiv: 1708.09079 [hep-ph].
Reimplemented from NPbase.
Definition at line 18383 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the anomalous triple gauge coupling \(\kappa_{Z}\).
Definition at line 18327 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(b\) quark, \(\delta m_b/m_b\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 4038 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(b\) quark squared, \((\delta m_b/m_b)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 4044 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(c\) quark, \(\delta m_c/m_c\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 4049 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(c\) quark squared, \((\delta m_c/m_c)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 4055 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(H\) boson, \(\delta M_H/M_H\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 4016 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(H\) boson squared, \((\delta M_H/M_H)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 4022 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaMLL2_f | ( | const Particle | f, |
| const double | s, | ||
| const double | t | ||
| ) | const |
Definition at line 26216 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaMLR2_f | ( | const Particle | f, |
| const double | s | ||
| ) | const |
Definition at line 25997 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaMLR2t_e | ( | const double | t | ) | const |
Definition at line 26169 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaMRL2_f | ( | const Particle | f, |
| const double | s | ||
| ) | const |
Definition at line 26083 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaMRL2t_e | ( | const double | t | ) | const |
Definition at line 26212 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::deltaMRR2_f | ( | const Particle | f, |
| const double | s, | ||
| const double | t | ||
| ) | const |
Definition at line 26311 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(t\) quark, \(\delta m_t/m_t\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 4027 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(t\) quark squared, \((\delta m_t/m_t)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 4033 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(\tau\) lepton, \(\delta m_\tau/m_\tau\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 4060 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(\tau\) lepton squared, \((\delta m_\tau/m_\tau)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 4066 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(W\) boson, \(\delta M_W/M_W\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 4115 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(W\) boson squared, \((\delta M_W/M_W)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 4122 of file NPSMEFTd6.cpp.
|
virtual |
The relative NP corrections to the mass of the \(W\) boson, \(\delta M_W/M_W\).
Definition at line 4196 of file NPSMEFTd6.cpp.
|
virtual |
The relative NP corrections to the mass of the \(W\) boson squared, \((\delta M_W/M_W)^2\).
Definition at line 4206 of file NPSMEFTd6.cpp.
|
virtual |
The relative \(\mathcal{O}(\Lambda^{-4})\) NP corrections to the mass of the \(W\) boson, \(\Delta M_W^{(2)}\).
\(\nc{\dGf}{\delta_{G_F}}\)
\[ \Delta M_W^{(2)} = \frac{\gwQ}{\gwt} + \frac{\dGf^{(2)}}{2} + \frac{\gwL \dGf^{(1)}}{2\gwt} - \frac{(\dGf^{(1)})^2}{8} \]
Definition at line 4213 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(Z\) boson, \(\delta M_Z/M_Z\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 4005 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(Z\) boson squared, \((\delta M_Z/M_Z)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 4011 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the cross section in pb for \(e^+ e^- \to W^+ W^- \to 4f \), with \( 4f = 0 (jjjj), 1 (e v jj), 2 (mu v jj), 3 (tau v jj), 4 (e v e v), 5 (mu v mu v), 6 (tau v tau v), 7 (e v mu v), 8 (e v tau v), 9 (mu v tau v), 10 (l v jj), 11 (l v l v) \) the different fermion final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph].
Reimplemented from NPbase.
Definition at line 18397 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the total cross section in pb for \(e^+ e^- \to W^+ W^-\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph].
Reimplemented from NPbase.
Definition at line 19501 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(\delta y_b\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 23681 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(\delta y_c\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 23701 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(\delta y_\mu\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 23720 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(\delta y_s\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 23711 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(\delta y_t\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 23671 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(\delta y_\tau\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 23691 of file NPSMEFTd6.cpp.
|
virtual |
The differential cross section in pb for \(e^+ e^- \to W^+ W^- \to lv jj \), with \( l= e,\mu \) for the 4 \( cos{\theta}\) bins defined in arXiv: 1606.06693 [hep-ph]. for the C.O.M. energies of 182.6 and 205.9 GeV. From arXiv: 1606.06693 [hep-ph].
Reimplemented from NPbase.
Definition at line 19895 of file NPSMEFTd6.cpp.
|
virtual |
The differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\), as a function of the \(W\) polar angle.
Reimplemented from NPbase.
Definition at line 20289 of file NPSMEFTd6.cpp.
|
virtual |
The integral of differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\) in a given bin of the \(W\) polar angle.
< Gsl integral variable
< Gsl integral variable
< Gsl integral variable
Reimplemented from NPbase.
Definition at line 20588 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::f_triangle | ( | double | tau | ) | const |
Loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings.
| [in] |
_form#4670, with \(M\) the mass of the particle in the loop.
Definition at line 5069 of file NPSMEFTd6.cpp.
| bool NPSMEFTd6::flagCHWpCHB | ( | ) | const |
If True, uses the coefficient CHWpCHW instead of the sum CiHW+CiHB.
Definition at line 3169 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::g_triangle | ( | double | tau | ) | const |
Loop function entering in the calculation of the effective \(HZ\gamma\) coupling.
| [in] |
_form#4670, with \(M\) the mass of the particle in the loop.
Definition at line 5081 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH2d2dRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2d2d)\) in the current model and in the Standard Model.
Definition at line 14423 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH2e2muRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2e 2\mu)\) in the current model and in the Standard Model.
Definition at line 13744 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH2e2vRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2e2v)\) in the current model and in the Standard Model.
Definition at line 14136 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH2evRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2ev)\) in the current model and in the Standard Model.
Definition at line 16389 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH2L2dRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2L2d)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Definition at line 14726 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH2L2LRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2L2L')\) ( \(L,L'=e,\mu,\tau\)) in the current model and in the Standard Model.
Definition at line 13646 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH2L2uRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2L2u)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Definition at line 14624 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH2L2v2Ratio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu\)) in the current model and in the Standard Model.
Definition at line 14036 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH2L2vRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2L2v)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Definition at line 13935 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH2l2vRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2l2v)\) ( \(l=e,\mu\)) in the current model and in the Standard Model.
Definition at line 16751 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH2Lv2Ratio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu\)) in the current model and in the Standard Model.
Definition at line 16287 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH2LvRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2Lv)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Definition at line 16182 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH2mu2vRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2\mu 2v)\) in the current model and in the Standard Model.
Definition at line 14232 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH2muvRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2\mu v)\) in the current model and in the Standard Model.
Definition at line 16487 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH2u2dRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2u2d)\) in the current model and in the Standard Model.
Definition at line 14521 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH2u2uRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2u2u)\) in the current model and in the Standard Model.
Definition at line 14327 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH2udRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2ud)\) in the current model and in the Standard Model.
Definition at line 16077 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH2v2dRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2v2d)\) in the current model and in the Standard Model.
Definition at line 14929 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH2v2uRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2v2u)\) in the current model and in the Standard Model.
Definition at line 14830 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH2v2vRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 2v2v)\) in the current model and in the Standard Model.
Definition at line 13840 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH4dRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 4d)\) in the current model and in the Standard Model.
Definition at line 15602 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH4eRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 4e)\) in the current model and in the Standard Model.
Definition at line 15224 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH4fRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 4f)\) in the current model and in the Standard Model.
Definition at line 16585 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH4L2Ratio | ( | ) | const |
The ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu\)) in the current model and in the Standard Model.
Definition at line 15128 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH4LRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 4L)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Definition at line 15030 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH4lRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 4l)\) ( \(l=e,\mu\)) in the current model and in the Standard Model.
Definition at line 16686 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH4muRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 4\mu)\) in the current model and in the Standard Model.
Definition at line 15317 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH4uRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 4u)\) in the current model and in the Standard Model.
Definition at line 15505 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaH4vRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to 4v)\) in the current model and in the Standard Model.
Definition at line 15410 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 13549 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 13458 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaHevmuvRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to e\nu \mu\nu)\) in the current model and in the Standard Model.
Definition at line 15795 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 13193 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 12632 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaHll_vvorjjRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to l l \nu\nu, l l j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model.
Definition at line 17085 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaHlv_lvorjjRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to l \nu l \nu, l \nu j j)\) ( \(l=e,\mu,~~j\not=b\)) in the current model and in the Standard Model.
Definition at line 17018 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaHlvjjRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to l l j j)\) ( \(l=e,\mu@f,~~j\not=b$) in the current model and in the Standard Model. @return \)\Gamma(H\to l l j j) \(/\)\Gamma(H\to l l j j)_{\mathrm{SM}} \( */ const double GammaHlljjRatio() const; /** @brief The new physics contribution to the ratio of the \)\Gamma(H\to l l j j) \( (\)l=e,\mu,~~j\not=b \() in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) @return \)\delta \Gamma(H\to l l j j) \(/\)\Gamma(H\to l l j j)_{\mathrm{SM}} \( */ const double deltaGammaHlljjRatio1() const; /** @brief The new physics contribution to the ratio of the \)\Gamma(H\to l l j j) \( (\)l=e,\mu,~~j\not=b \() in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) @return \)\delta \Gamma(H\to l l j j) \(/\)\Gamma(H\to l l j j)_{\mathrm{SM}} \( */ const double deltaGammaHlljjRatio2() const; /** @brief The ratio of the Br\)(H\to l l j j) \( (\)l=e,\mu,~~j\not=b \() in the current model and in the Standard Model. @return Br\)(H\to l l j j) \(/Br\)(H\to l l j j)_{\mathrm{SM}} \( */ virtual const double BrHlljjRatio() const; /** @brief The ratio of the \)\Gamma(H\to l \nu j j) \( (\)l=e,\mu@f,~~j\not=b$) in the current model and in the Standard Model.
Definition at line 16923 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaHLvudRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Lvud)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Definition at line 15981 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaHLvvLRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to LvvL)\) ( \(L=e,\mu,\tau\)) in the current model and in the Standard Model.
Definition at line 15701 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 13303 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 13380 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaHudduRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to uddu)\) in the current model and in the Standard Model.
Definition at line 15888 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaHWW4fRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 12782 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 12727 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 13046 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::GammaHZZ4fRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 12929 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 12876 of file NPSMEFTd6.cpp.
|
virtual |
The total width of the \(W\) boson, \(\Gamma_W\).
Reimplemented from NPbase.
Definition at line 4357 of file NPSMEFTd6.cpp.
A partial decay width of the \(W\) boson decay into a SM fermion pair.
| [in] | fi | a lepton or quark |
| [in] | fj | a lepton or quark |
Reimplemented from NPbase.
Definition at line 4292 of file NPSMEFTd6.cpp.
|
inline |
|
inline |
|
inline |
|
inline |
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inline |
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inline |
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inline |
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inline |
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inline |
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inline |
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inline |
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inline |
|
inline |
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inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inlinevirtual |
A method to get the Matching object for this model.
Reimplemented from StandardModel.
Definition at line 1128 of file NPSMEFTd6.h.
| bool NPSMEFTd6::hatCis | ( | ) | const |
If True, explicitly defines the 8 'hat' coefficients in the EWPOs (Z-couplings, dGf, W-width)
Definition at line 3164 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::I_triangle_1 | ( | double | tau, |
| double | lambda | ||
| ) | const |
Loop function entering in the calculation of the effective \(HZ\gamma\) coupling.
| [in] |
_form#4670, \(\lambda=4 M^2/m_Z^2\), with \(M\) the mass of the particle in the loop.
Definition at line 5093 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::I_triangle_2 | ( | double | tau, |
| double | lambda | ||
| ) | const |
Loop function entering in the calculation of the effective \(HZ\gamma\) coupling.
| [in] |
_form#4670, \(\lambda=4 M^2/m_Z^2\), with \(M\) the mass of the particle in the loop.
Definition at line 5104 of file NPSMEFTd6.cpp.
|
virtual |
Definition at line 26701 of file NPSMEFTd6.cpp.
|
virtual |
Definition at line 26781 of file NPSMEFTd6.cpp.
|
virtual |
Definition at line 26763 of file NPSMEFTd6.cpp.
|
virtual |
Definition at line 26808 of file NPSMEFTd6.cpp.
|
virtual |
Definition at line 26772 of file NPSMEFTd6.cpp.
|
virtual |
Definition at line 26732 of file NPSMEFTd6.cpp.
|
virtual |
Definition at line 26650 of file NPSMEFTd6.cpp.
|
virtual |
Definition at line 26606 of file NPSMEFTd6.cpp.
|
virtual |
Definition at line 26632 of file NPSMEFTd6.cpp.
|
virtual |
Definition at line 26675 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{A,eff}=\sqrt{\Gamma_{HAA}/\Gamma_{HAA}^{SM}}\).
Reimplemented from NPbase.
Definition at line 23658 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{b,eff}=\sqrt{\Gamma_{Hbb}/\Gamma_{Hbb}^{SM}}\).
Reimplemented from NPbase.
Definition at line 23638 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{c,eff}=\sqrt{\Gamma_{Hcc}/\Gamma_{Hcc}^{SM}}\).
Reimplemented from NPbase.
Definition at line 23633 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{G,eff}=\sqrt{\Gamma_{HGG}/\Gamma_{HGG}^{SM}}\).
Reimplemented from NPbase.
Definition at line 23643 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{\mu,eff}=\sqrt{\Gamma_{H\mu\mu}/\Gamma_{H\mu\mu}^{SM}}\).
Reimplemented from NPbase.
Definition at line 23623 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{\tau,eff}=\sqrt{\Gamma_{H\tau\tau}/\Gamma_{H\tau\tau}^{SM}}\).
Reimplemented from NPbase.
Definition at line 23628 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{W,eff}=\sqrt{\Gamma_{HWW}/\Gamma_{HWW}^{SM}}\).
Reimplemented from NPbase.
Definition at line 23653 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{ZA,eff}=\sqrt{\Gamma_{HZA}/\Gamma_{HZA}^{SM}}\).
Reimplemented from NPbase.
Definition at line 23663 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{Z,eff}=\sqrt{\Gamma_{HZZ}/\Gamma_{HZZ}^{SM}}\).
Reimplemented from NPbase.
Definition at line 23648 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the anomalous triple gauge coupling \(\lambda_{Z}\).
Reimplemented from NPbase.
Definition at line 18358 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(\lambda_{z}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
| [in] | mu | the RG scale to be used in the evaluation |
Reimplemented from NPbase.
Definition at line 23808 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 5901 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Definition at line 6239 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 11292 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Definition at line 11493 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 5605 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeWW}\) between the \( e^{+}e^{-}\to W^{+}W^{-} \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 20638 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeWW}\) between the \( e^{+}e^{-}\to W^{+}W^{-} \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Definition at line 20796 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 7269 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Definition at line 7586 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeZH}\) between the \(e^{+}e^{-}\to ZH\) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 9333 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeZH}\) between the \( e^{+}e^{-}\to ZH \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Definition at line 9698 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 9649 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Definition at line 10684 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 9671 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Definition at line 10704 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{epWBF}\) between the \( e^{-} p\to \nu j H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 8573 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{epZBF}\) between the \( e^{-} p\to e^{-} j H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 8667 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 5200 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17637 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17349 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggHH}\) between the gluon-gluon fusion di-Higgs production cross-section in the current model and in the Standard Model. (From arXiv: 1502.00539 [hpe-ph].)
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 5215 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17565 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH+ttH}\) between the sum of gluon-gluon fusion and t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11278 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17601 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17493 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17529 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17385 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17421 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17457 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12151 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{\mu\mu H\mu\mu}\) between the \(\sigma(\mu \mu \to H \mu \mu)}\) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12363 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model, in the narrow width approximation.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12169 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{\mu\mu H\nu\nu}\) between the \(\sigma(\mu \mu \to H \nu \nu)}\) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12273 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{\mu\mu ttH}\) between the \(\sigma(\mu \mu \to t\bar{t} H )}\) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12448 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{\mu\mu ZH}\) between the \(\sigma(\mu \mu \to Z H)}\) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12189 of file NPSMEFTd6.cpp.
|
virtual |
The number of events in \( p p \to WZ\) in a given \(p_{TV}\) bin, normalized to the SM prediction. From arXiv: 1712.01310 [hep-ph] and private communication. Implemented only in NPSMEFTd6 class.
Reimplemented from NPbase.
Definition at line 21334 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{tHq}\) between the t-q-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11185 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18183 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17679 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18057 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18120 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17931 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17994 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17742 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,Z\gamma\to \gamma 2\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\to \gamma 2\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18297 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17805 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17868 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,ZZ\to 4\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18288 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18237 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17733 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18111 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18174 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17985 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18048 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17796 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17859 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17922 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF}\) between the VBF production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18246 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18192 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17688 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,inv}\) between the VBF production cross-section with subsequent decay into invisible states in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18251 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18066 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18129 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17940 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18003 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17751 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17814 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17877 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18219 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH}\) between the VH production cross-section in the current model and in the Standard Model, multiplied by the total (SM+new physics) invisible decay branching ratio.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18260 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17715 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,inv}\) between the VH production cross-section with subsequent decay into invisible states in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18272 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18093 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18156 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17967 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18030 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17778 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17841 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17904 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18210 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17706 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18084 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18147 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17958 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18021 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17769 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17832 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17895 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18201 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17697 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18075 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18138 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17949 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 18012 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17760 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17823 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17886 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11170 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17667 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17379 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H\to b\bar{b}\), \(Z\to e^+e^-\) channel channel in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17294 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17595 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17631 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17523 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17559 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H,Z\to b\bar{b}\) channel in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17239 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17415 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17451 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17487 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 5542 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF+\gamma}\) between the vector-boson fusion Higgs production cross-section in association with a hard photon in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 5557 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17643 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17355 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17571 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17607 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17499 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17535 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17391 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17427 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17463 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF+VH}\) between the sum of VBF and WH+ZH associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 10880 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 10851 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17661 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17373 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17589 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model, with \(p_{T,H}>250\) GeV.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 10866 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17625 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17517 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17553 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17409 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17445 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17481 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 8972 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17655 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17367 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17583 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model, with \(p_{T,H}>250\) GeV.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 8987 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17619 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17511 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17547 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17403 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17439 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17475 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 9265 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17649 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17361 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17577 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model, with \(p_{T,H}>250\) GeV.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 9280 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17613 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17505 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17541 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17397 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17433 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 17469 of file NPSMEFTd6.cpp.
|
virtual |
The mass of the \(W\) boson, \(M_W\).
\[ M_W = M_W^{SM}( 1 + \Delta M_W^{(1)} + \Delta M_W^{(2)}) \]
Reimplemented from NPbase.
Definition at line 4171 of file NPSMEFTd6.cpp.
|
virtual |
Number of di-electron events at the LHC at 13 TeV.
Reimplemented from NPbase.
Definition at line 23932 of file NPSMEFTd6.cpp.
|
virtual |
Number of mono-electron events at the LHC at 13 TeV.
Reimplemented from NPbase.
Definition at line 24109 of file NPSMEFTd6.cpp.
|
virtual |
Number of di-muon events at the LHC at 13 TeV.
Reimplemented from NPbase.
Definition at line 24007 of file NPSMEFTd6.cpp.
|
virtual |
Number of mono-muon events at the LHC at 13 TeV.
Reimplemented from NPbase.
Definition at line 24161 of file NPSMEFTd6.cpp.
|
virtual |
Number of mono-tau events at the LHC at 13 TeV.
Reimplemented from NPbase.
Definition at line 24209 of file NPSMEFTd6.cpp.
|
virtual |
Number of di-tau events at the LHC at 13 TeV.
Reimplemented from NPbase.
Definition at line 24065 of file NPSMEFTd6.cpp.
|
virtual |
The oblique parameter \(S\). (Simplified implementation. Contribution only from \(O_{HWB}\).)
Reimplemented from NPbase.
Definition at line 3978 of file NPSMEFTd6.cpp.
|
virtual |
The oblique parameter \(T\). (Simplified implementation. Contribution only from \(O_{HD}\).)
Reimplemented from NPbase.
Definition at line 3983 of file NPSMEFTd6.cpp.
|
virtual |
The oblique parameter \(U\).
Reimplemented from NPbase.
Definition at line 3988 of file NPSMEFTd6.cpp.
|
virtual |
The oblique parameter \(W\). (Simplified implementation. Contribution only from \(O_{2W}\).)
Reimplemented from NPbase.
Definition at line 3993 of file NPSMEFTd6.cpp.
|
virtual |
The oblique parameter \(Y\). (Simplified implementation. Contribution only from \(O_{2B}\).)
Reimplemented from NPbase.
Definition at line 3998 of file NPSMEFTd6.cpp.
|
virtual |
Type of contributions to be included in the EWPOs. Takes a numerica values depending on the choice.
Reimplemented from NPbase.
Definition at line 3154 of file NPSMEFTd6.cpp.
|
virtual |
The post-update method for NPSMEFTd6.
This method runs all the procedures that are need to be executed after the model is successfully updated.
Reimplemented from StandardModel.
Definition at line 1088 of file NPSMEFTd6.cpp.
|
virtual |
The direction constrained by \( p p \to Z H\) in the boosted regime, \(g_p^Z\). From arXiv:1807.01796 and the contribution to FCC CDR Vol 1. Implemented only in NPSMEFTd6 class.
Reimplemented from NPbase.
Definition at line 21298 of file NPSMEFTd6.cpp.
|
virtual |
A function to apply the 1st leading log corrections to the Wilson coefficients, according to the d6 SMEFT RGEs.
This method runs inside the PostUpdate() method, after the definition of the internal Ci coefficients, adding the log corrections according to the d6 SMEFT RGEs. It also sets the values of the corresponding anomalous dimensions.
Definition at line 3176 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \( R_{W,c}=\Gamma(W\to c + X)/\Gamma(W\to had) \).
Reimplemented from NPbase.
Definition at line 4636 of file NPSMEFTd6.cpp.
The lepton universality ratio \(R_{W,l_i/l_j)=\Gamma(W\to l_i \nu_i)/\Gamma(W\to l_j \nu_j)\).
\[ RWc = RWc^{SM} + \Delta RWc^{(1)} + \Delta RWc^{(2)} \]
where,
\[ \Delta RWc^{(2)} = \frac{\Delta \Gamma_{W,cx}^{(2)}}{\Gamma_{W,had}^{SM}} + \frac{\Gamma_{W,cx}^{SM} ~\Delta \Gamma_{W,had}^{(1)}}{\Gamma_{W,had}^{SM}} + \frac{\Gamma_{W,cx}^{SM} ~(\Delta \Gamma_{W,had}^{(1)})^2}{(\Gamma_{W,had}^{SM})^3} - \frac{\Delta \Gamma_{W,cx}^{(1)} ~\Delta \Gamma_{W,had}^{(1)}}{(\Gamma_{W,had}^{SM})^2} \]
Reimplemented from NPbase.
Definition at line 4602 of file NPSMEFTd6.cpp.
The lepton universality ratio \(R_{Z,l_i/l_j)=\Gamma(Z\to l_i^+ l_i^-)/\Gamma(Z\to l_j^+ l_j^-)\).
Reimplemented from NPbase.
Definition at line 4696 of file NPSMEFTd6.cpp.
|
virtual |
A method to set a flag of NPSMEFTd6.
| [in] | name | name of a model flag |
| [in] | value | the boolean to be assigned to the flag specified by name |
Reimplemented from NPbase.
Definition at line 3089 of file NPSMEFTd6.cpp.
|
protectedvirtual |
A method to set the value of a parameter of the model.
| [in] | name | name of a model parameter |
| [in] | value | the value to be assigned to the parameter specified by name |
Reimplemented from StandardModel.
Definition at line 1493 of file NPSMEFTd6.cpp.
|
virtual |
Reimplemented from NPbase.
Definition at line 26836 of file NPSMEFTd6.cpp.
|
virtual |
The STXS0 bin \(pp \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21439 of file NPSMEFTd6.cpp.
|
virtual |
The STXS BR \( H \to 4l \), \(l=e,\mu\).
Reimplemented from NPbase.
Definition at line 22101 of file NPSMEFTd6.cpp.
|
virtual |
The STXS BR \( H \to bb \).
Reimplemented from NPbase.
Definition at line 22172 of file NPSMEFTd6.cpp.
|
virtual |
The STXS BR \( H \to e\nu \mu\nu \).
Reimplemented from NPbase.
Definition at line 22125 of file NPSMEFTd6.cpp.
|
virtual |
The STXS BR \( H \to \gamma \gamma \).
Reimplemented from NPbase.
Definition at line 22147 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j \geq 2,~m_{jj}[GeV]<350,~p_{TH} [GeV]<60\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22420 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j \geq 2,~m_{jj}[GeV]<350,~120<p_{TH} [GeV]<200\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22470 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j \geq 2,~m_{jj}[GeV]<350,~60<p_{TH} [GeV]<120\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22445 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH} [GeV]<200,~p_{THjj}[GeV]<25\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22495 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH} [GeV]<200,~25<p_{THjj}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22520 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200,~p_{THjj}[GeV]<25\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22545 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH} [GeV]<200,~25<p_{THjj}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22570 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j=0,~p_{TH} [GeV]<10\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22295 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j = 1,~p_{TH} [GeV]<60\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22345 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j=0,~10<p_{TH} [GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22320 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j = 1,~120<p_{TH} [GeV]<200\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22395 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j\leq 1,~200<p_{TH} [GeV]<300\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22195 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j\leq 1,~300<p_{TH} [GeV]<450\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22220 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j\leq 1,~450<p_{TH} [GeV]<650\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22245 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j = 1,~60<p_{TH} [GeV]<120\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22370 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\), \(N_j\leq 1,650<p_{TH} [GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22270 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\ell\ell\), \(p_{TV}[GeV]<75\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22595 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\ell\ell\), \(N_j = 0,~150<p_{TV}[GeV]<250\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22667 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\ell\ell\), \(N_j = 1,~150<p_{TV}[GeV]<250\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22702 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\ell\ell\), \(250 < p_{TV}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22737 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\ell\ell\), \(75<p_{TV}[GeV]<150\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22631 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\ell\), \(p_{TV}[GeV]<75\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 23234 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\ell\), \(N_j = 0,~150<p_{TV}[GeV]<250\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 23300 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\ell\), \(N_j \geq 1,~150<p_{TV}[GeV]<250\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 23333 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\ell\), \(250<p_{TV}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 23366 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\ell\), \(75<p_{TV}[GeV]<150\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 23267 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\nu\), \(p_{TV}[GeV]<75\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 23094 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\nu\), \(N_j = 0,~150<p_{TV}[GeV]<250\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 23150 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\nu\), \(N_j \geq 1,~150<p_{TV}[GeV]<250\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 23178 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\nu\), \(250<p_{TV}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 23206 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H\ell\nu\), \(75<p_{TV}[GeV]<150\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 23122 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~m_{jj}[GeV]<60\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22836 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~120<m_{jj}[GeV]<350\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22901 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200,~p_{THjj}[GeV]<25\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22965 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV]<700,~p_{TH}[GeV]<200,~25<p_{THjj}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22998 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~350<m_{jj}[GeV],~200<p_{TH}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22933 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~60<m_{jj}[GeV]<120\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22869 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH}[GeV]<200,~p_{THjj}[GeV]<25\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 23030 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j \geq 2,~700<m_{jj}[GeV],~p_{TH}[GeV]<200,~25<p_{THjj}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 23062 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j = 0\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22771 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to Hqq\), \(N_j = 1\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22804 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(pp \to tH\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 23589 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(pp \to ttH\), \(p_{TH}[GeV]<60\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 23399 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(pp \to ttH\), \(120<p_{TH}[GeV]<200\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 23473 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(pp \to ttH\), \(200<p_{TH}[GeV]<300\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 23510 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(pp \to ttH\), \(300<p_{TH}[GeV]\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 23548 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(pp \to ttH\), \(60<p_{TH}[GeV]<120\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 23436 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21527 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21542 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21572 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21587 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21557 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21602 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21614 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21638 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21650 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21626 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21515 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(gg \to H\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21503 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \ell\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21843 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \ell\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21867 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \ell\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21887 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \ell\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21901 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \ell\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21915 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \nu\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21787 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \nu\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21770 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \nu\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21799 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \nu\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21811 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H \ell \nu\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21823 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21695 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21749 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21737 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21683 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21671 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21665 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \(qq \to H qq\).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21716 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \( ttH + tH \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21939 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \( qq \to WH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22018 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \( qq \to WH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22006 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \( qq \to WH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21982 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \( qq \to WH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21970 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \( qq \to WH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 21994 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \( qq \to ZH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22082 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \( qq \to ZH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22069 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \( qq \to ZH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22043 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \( qq \to ZH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22030 of file NPSMEFTd6.cpp.
|
virtual |
The STXS bin \( qq \to ZH \to H qq \).
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 22056 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::tovers2 | ( | const double | cosmin, |
| const double | cosmax | ||
| ) | const |
Definition at line 26408 of file NPSMEFTd6.cpp.
| const double NPSMEFTd6::uovers2 | ( | const double | cosmin, |
| const double | cosmax | ||
| ) | const |
Definition at line 26412 of file NPSMEFTd6.cpp.
|
virtual |
Total \(e^+ e^- \to W^+ W^- \to jj \ell \nu\) cross section in pb, with \(\ell= e, \mu\).
Reimplemented from NPbase.
Definition at line 20633 of file NPSMEFTd6.cpp.
|
virtual |
The cross section in pb for \(e^+ e^- \to W^+ W^- \to 4f \), with \( 4f = 0 (jjjj), 1 (e v jj), 2 (mu v jj), 3 (tau v jj), 4 (e v e v), 5 (mu v mu v), 6 (tau v tau v), 7 (e v mu v), 8 (e v tau v), 9 (mu v tau v), 10 (l v jj), 11 (l v l v) \) the different fermion final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph].
Reimplemented from NPbase.
Definition at line 18961 of file NPSMEFTd6.cpp.
|
virtual |
The total cross section in pb for \(e^+ e^- \to W^+ W^-\), summing over all final states for C.O.M. energies in 188-208 GeV. From arXiv: 1606.06693 [hep-ph].
Reimplemented from NPbase.
Definition at line 19506 of file NPSMEFTd6.cpp.
|
protected |
Definition at line 6964 of file NPSMEFTd6.h.
|
protected |
Definition at line 6964 of file NPSMEFTd6.h.
|
protected |
Definition at line 6966 of file NPSMEFTd6.h.
|
protected |
Definition at line 6965 of file NPSMEFTd6.h.
|
protected |
Definition at line 6964 of file NPSMEFTd6.h.
|
protected |
Definition at line 6965 of file NPSMEFTd6.h.
|
protected |
Definition at line 6965 of file NPSMEFTd6.h.
|
protected |
Definition at line 6967 of file NPSMEFTd6.h.
|
protected |
Definition at line 6967 of file NPSMEFTd6.h.
|
protected |
Definition at line 6967 of file NPSMEFTd6.h.
|
protected |
Definition at line 6967 of file NPSMEFTd6.h.
|
protected |
Definition at line 6967 of file NPSMEFTd6.h.
|
protected |
Definition at line 6965 of file NPSMEFTd6.h.
|
protected |
Definition at line 6967 of file NPSMEFTd6.h.
|
protected |
Definition at line 6967 of file NPSMEFTd6.h.
|
protected |
Definition at line 6965 of file NPSMEFTd6.h.
|
protected |
Definition at line 6968 of file NPSMEFTd6.h.
|
protected |
Definition at line 6968 of file NPSMEFTd6.h.
|
protected |
Definition at line 6965 of file NPSMEFTd6.h.
|
protected |
The em constant at Mz.
Definition at line 6912 of file NPSMEFTd6.h.
|
protected |
The branching ratio of exotic (not invisible) Higgs decays.
Definition at line 6763 of file NPSMEFTd6.h.
|
protected |
The branching ratio of invisible Higgs decays.
Definition at line 6762 of file NPSMEFTd6.h.
|
protected |
The C1 coefficient controlling the H^3 corrections to the total Higgs width from the Higgs trilinear coupling.
Definition at line 6986 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{2W}\).
Definition at line 6313 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{2W}^{SILH}\).
Definition at line 6315 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{2B}\).
Definition at line 6314 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{2B}^{SILH}\).
Definition at line 6316 of file NPSMEFTd6.h.
|
protected |
Definition at line 6957 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{DB}\).
Definition at line 6324 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dB})_{11}\) (imaginary part).
Definition at line 6508 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dB})_{11}\) (real part).
Definition at line 6502 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dB})_{12}\) (imaginary part).
Definition at line 6509 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dB})_{12}\) (real part).
Definition at line 6503 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dB})_{13}\) (imaginary part).
Definition at line 6510 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dB})_{13}\) (real part).
Definition at line 6504 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dB})_{22}\) (imaginary part).
Definition at line 6511 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dB})_{22}\) (real part).
Definition at line 6505 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dB})_{23}\) (imaginary part).
Definition at line 6512 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dB})_{23}\) (real part).
Definition at line 6506 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dB})_{33}\) (imaginary part).
Definition at line 6513 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dB})_{33}\) (real part).
Definition at line 6507 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dG})_{11}\) (imaginary part).
Definition at line 6484 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dG})_{11}\) (real part).
Definition at line 6478 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dG})_{12}\) (imaginary part).
Definition at line 6485 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dG})_{12}\) (real part).
Definition at line 6479 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dG})_{13}\) (imaginary part).
Definition at line 6486 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dG})_{13}\) (real part).
Definition at line 6480 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dG})_{22}\) (imaginary part).
Definition at line 6487 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dG})_{22}\) (real part).
Definition at line 6481 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dG})_{23}\) (imaginary part).
Definition at line 6488 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dG})_{23}\) (real part).
Definition at line 6482 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dG})_{33}\) (imaginary part).
Definition at line 6489 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dG})_{33}\) (real part).
Definition at line 6483 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{11}\) (imaginary part).
Definition at line 6436 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{11}\) (real part).
Definition at line 6430 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{12}\) (imaginary part).
Definition at line 6437 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{12}\) (real part).
Definition at line 6431 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{13}\) (imaginary part).
Definition at line 6438 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{13}\) (real part).
Definition at line 6432 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{22}\) (imaginary part).
Definition at line 6439 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{22}\) (real part).
Definition at line 6433 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{23}\) (imaginary part).
Definition at line 6440 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{23}\) (real part).
Definition at line 6434 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{33}\) (imaginary part).
Definition at line 6441 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{33}\) (real part).
Definition at line 6435 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{DHB}\).
Definition at line 6322 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{DHW}\).
Definition at line 6323 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{DW}\).
Definition at line 6325 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dW})_{11}\) (imaginary part).
Definition at line 6496 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dW})_{11}\) (real part).
Definition at line 6490 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dW})_{12}\) (imaginary part).
Definition at line 6497 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dW})_{12}\) (real part).
Definition at line 6491 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dW})_{13}\) (imaginary part).
Definition at line 6498 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dW})_{13}\) (real part).
Definition at line 6492 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dW})_{22}\) (imaginary part).
Definition at line 6499 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dW})_{22}\) (real part).
Definition at line 6493 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dW})_{23}\) (imaginary part).
Definition at line 6500 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dW})_{23}\) (real part).
Definition at line 6494 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dW})_{33}\) (imaginary part).
Definition at line 6501 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dW})_{33}\) (real part).
Definition at line 6495 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eB})_{11}\) (imaginary part).
Definition at line 6532 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eB})_{11}\) (real part).
Definition at line 6526 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eB})_{12}\) (imaginary part).
Definition at line 6533 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eB})_{12}\) (real part).
Definition at line 6527 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eB})_{13}\) (imaginary part).
Definition at line 6534 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eB})_{13}\) (real part).
Definition at line 6528 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eB})_{22}\) (imaginary part).
Definition at line 6535 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eB})_{22}\) (real part).
Definition at line 6529 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eB})_{23}\) (imaginary part).
Definition at line 6536 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eB})_{23}\) (real part).
Definition at line 6530 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eB})_{33}\) (imaginary part).
Definition at line 6537 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eB})_{33}\) (real part).
Definition at line 6531 of file NPSMEFTd6.h.
|
protected |
Definition at line 6558 of file NPSMEFTd6.h.
|
protected |
Definition at line 6559 of file NPSMEFTd6.h.
|
protected |
Definition at line 6561 of file NPSMEFTd6.h.
|
protected |
Definition at line 6562 of file NPSMEFTd6.h.
|
protected |
Definition at line 6560 of file NPSMEFTd6.h.
|
protected |
Definition at line 6559 of file NPSMEFTd6.h.
|
protected |
Definition at line 6561 of file NPSMEFTd6.h.
|
protected |
Definition at line 6562 of file NPSMEFTd6.h.
|
protected |
Definition at line 6560 of file NPSMEFTd6.h.
|
protected |
Definition at line 6561 of file NPSMEFTd6.h.
|
protected |
Definition at line 6562 of file NPSMEFTd6.h.
|
protected |
Definition at line 6551 of file NPSMEFTd6.h.
|
protected |
Definition at line 6552 of file NPSMEFTd6.h.
|
protected |
Definition at line 6553 of file NPSMEFTd6.h.
|
protected |
Definition at line 6552 of file NPSMEFTd6.h.
|
protected |
Definition at line 6553 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{11}\) (imaginary part).
Definition at line 6412 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{11}\) (real part).
Definition at line 6406 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{12}\) (imaginary part).
Definition at line 6413 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{12}\) (real part).
Definition at line 6407 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{13}\) (imaginary part).
Definition at line 6414 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{13}\) (real part).
Definition at line 6408 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{22}\) (imaginary part).
Definition at line 6415 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{22}\) (real part).
Definition at line 6409 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{23}\) (imaginary part).
Definition at line 6416 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{23}\) (real part).
Definition at line 6410 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{33}\) (imaginary part).
Definition at line 6417 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{33}\) (real part).
Definition at line 6411 of file NPSMEFTd6.h.
|
protected |
Definition at line 6554 of file NPSMEFTd6.h.
|
protected |
Definition at line 6555 of file NPSMEFTd6.h.
|
protected |
Definition at line 6556 of file NPSMEFTd6.h.
|
protected |
Definition at line 6555 of file NPSMEFTd6.h.
|
protected |
Definition at line 6557 of file NPSMEFTd6.h.
|
protected |
Definition at line 6556 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eW})_{11}\) (imaginary part).
Definition at line 6520 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eW})_{11}\) (real part).
Definition at line 6514 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eW})_{12}\) (imaginary part).
Definition at line 6521 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eW})_{12}\) (real part).
Definition at line 6515 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eW})_{13}\) (imaginary part).
Definition at line 6522 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eW})_{13}\) (real part).
Definition at line 6516 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eW})_{22}\) (imaginary part).
Definition at line 6523 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eW})_{22}\) (real part).
Definition at line 6517 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eW})_{23}\) (imaginary part).
Definition at line 6524 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eW})_{23}\) (real part).
Definition at line 6518 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eW})_{33}\) (imaginary part).
Definition at line 6525 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eW})_{33}\) (real part).
Definition at line 6519 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{G}\).
Definition at line 6311 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{H}\).
Definition at line 6330 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{HB}\).
Definition at line 6319 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{H\Box}\).
Definition at line 6329 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{HD}\).
Definition at line 6327 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{11}\).
Definition at line 6385 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{12}\) (imaginary part).
Definition at line 6391 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{12}\) (real part).
Definition at line 6386 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{13}\) (imaginary part).
Definition at line 6392 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{13}\) (real part).
Definition at line 6387 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{22}\).
Definition at line 6388 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{23}\) (imaginary part).
Definition at line 6393 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{23}\) (real part).
Definition at line 6389 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{33}\).
Definition at line 6390 of file NPSMEFTd6.h.
|
protected |
Definition at line 6305 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{11}\).
Definition at line 6349 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{12}\) (imaginary part).
Definition at line 6355 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{12}\) (real part).
Definition at line 6350 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{13}\) (imaginary part).
Definition at line 6356 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{13}\) (real part).
Definition at line 6351 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{22}\).
Definition at line 6352 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{23}\) (imaginary part).
Definition at line 6357 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{23}\) (real part).
Definition at line 6353 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{33}\).
Definition at line 6354 of file NPSMEFTd6.h.
|
protected |
Definition at line 6307 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{HG}\).
Definition at line 6317 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{11}\).
Definition at line 6331 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (imaginary part).
Definition at line 6337 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (real part).
Definition at line 6332 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (imaginary part).
Definition at line 6338 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (real part).
Definition at line 6333 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{22}\).
Definition at line 6334 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (imaginary part).
Definition at line 6339 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (real part).
Definition at line 6335 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{33}\).
Definition at line 6336 of file NPSMEFTd6.h.
|
protected |
Definition at line 6301 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{11}\).
Definition at line 6340 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part).
Definition at line 6346 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part).
Definition at line 6341 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part).
Definition at line 6347 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part).
Definition at line 6342 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{22}\).
Definition at line 6343 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part).
Definition at line 6348 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part).
Definition at line 6344 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{33}\).
Definition at line 6345 of file NPSMEFTd6.h.
|
protected |
Definition at line 6302 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{11}\).
Definition at line 6358 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (imaginary part).
Definition at line 6364 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (real part).
Definition at line 6359 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (imaginary part).
Definition at line 6365 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (real part).
Definition at line 6360 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{22}\).
Definition at line 6361 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (imaginary part).
Definition at line 6366 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (real part).
Definition at line 6362 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{33}\).
Definition at line 6363 of file NPSMEFTd6.h.
|
protected |
Definition at line 6303 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{11}\).
Definition at line 6367 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (imaginary part).
Definition at line 6373 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (real part).
Definition at line 6368 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (imaginary part).
Definition at line 6374 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (real part).
Definition at line 6369 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{22}\).
Definition at line 6370 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (imaginary part).
Definition at line 6375 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (real part).
Definition at line 6371 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{33}\).
Definition at line 6372 of file NPSMEFTd6.h.
|
protected |
Definition at line 6304 of file NPSMEFTd6.h.
|
protected |
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes.
Definition at line 6948 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{11}\).
Definition at line 6376 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{12}\) (imaginary part).
Definition at line 6382 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{12}\) (real part).
Definition at line 6377 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{13}\) (imaginary part).
Definition at line 6383 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{13}\) (real part).
Definition at line 6378 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{22}\).
Definition at line 6379 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{23}\) (imaginary part).
Definition at line 6384 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{23}\) (real part).
Definition at line 6380 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{33}\).
Definition at line 6381 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{11}\) (imaginary part).
Definition at line 6400 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{11}\) (real part).
Definition at line 6394 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{12}\) (imaginary part).
Definition at line 6401 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{12}\) (real part).
Definition at line 6395 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{13}\) (imaginary part).
Definition at line 6402 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{13}\) (real part).
Definition at line 6396 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{22}\) (imaginary part).
Definition at line 6403 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{22}\) (real part).
Definition at line 6397 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{23}\) (imaginary part).
Definition at line 6404 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{23}\) (real part).
Definition at line 6398 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{33}\) (imaginary part).
Definition at line 6405 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{33}\) (real part).
Definition at line 6399 of file NPSMEFTd6.h.
|
protected |
Definition at line 6306 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{HW}\).
Definition at line 6318 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{HWB}\).
Definition at line 6326 of file NPSMEFTd6.h.
|
protected |
The combination of dimension-6 operator coefficients entering in \(\delta_{AA}\): \(s_W^2 C_{HW} + c_W^2 C_{HW}\).
Definition at line 6320 of file NPSMEFTd6.h.
|
protected |
The combination of dimension-6 operator coefficients \(-c_W^2 C_{HW} + s_W^2 C_{HW}\).
Definition at line 6321 of file NPSMEFTd6.h.
|
protected |
Definition at line 6309 of file NPSMEFTd6.h.
|
protected |
Definition at line 6873 of file NPSMEFTd6.h.
|
protected |
Definition at line 6874 of file NPSMEFTd6.h.
|
protected |
Definition at line 6875 of file NPSMEFTd6.h.
|
protected |
Definition at line 6839 of file NPSMEFTd6.h.
|
protected |
Definition at line 6840 of file NPSMEFTd6.h.
|
protected |
Definition at line 6857 of file NPSMEFTd6.h.
|
protected |
Definition at line 6858 of file NPSMEFTd6.h.
|
protected |
Definition at line 6859 of file NPSMEFTd6.h.
|
protected |
Definition at line 6830 of file NPSMEFTd6.h.
|
protected |
Definition at line 6851 of file NPSMEFTd6.h.
|
protected |
Definition at line 6837 of file NPSMEFTd6.h.
|
protected |
Definition at line 6849 of file NPSMEFTd6.h.
|
protected |
Definition at line 6850 of file NPSMEFTd6.h.
|
protected |
Definition at line 6821 of file NPSMEFTd6.h.
|
protected |
Definition at line 6822 of file NPSMEFTd6.h.
|
protected |
Definition at line 6823 of file NPSMEFTd6.h.
|
protected |
Definition at line 6805 of file NPSMEFTd6.h.
|
protected |
Definition at line 6806 of file NPSMEFTd6.h.
|
protected |
Definition at line 6807 of file NPSMEFTd6.h.
|
protected |
Definition at line 6835 of file NPSMEFTd6.h.
|
protected |
Definition at line 6777 of file NPSMEFTd6.h.
|
protected |
Definition at line 6778 of file NPSMEFTd6.h.
|
protected |
Definition at line 6779 of file NPSMEFTd6.h.
|
protected |
Definition at line 6780 of file NPSMEFTd6.h.
|
protected |
Definition at line 6781 of file NPSMEFTd6.h.
|
protected |
Definition at line 6782 of file NPSMEFTd6.h.
|
protected |
Definition at line 6791 of file NPSMEFTd6.h.
|
protected |
Definition at line 6792 of file NPSMEFTd6.h.
|
protected |
Definition at line 6793 of file NPSMEFTd6.h.
|
protected |
Definition at line 6794 of file NPSMEFTd6.h.
|
protected |
Definition at line 6795 of file NPSMEFTd6.h.
|
protected |
Definition at line 6796 of file NPSMEFTd6.h.
|
protected |
Definition at line 6813 of file NPSMEFTd6.h.
|
protected |
Definition at line 6814 of file NPSMEFTd6.h.
|
protected |
Definition at line 6815 of file NPSMEFTd6.h.
|
protected |
Definition at line 6836 of file NPSMEFTd6.h.
|
protected |
Definition at line 6838 of file NPSMEFTd6.h.
|
protected |
Definition at line 6905 of file NPSMEFTd6.h.
|
protected |
Definition at line 6906 of file NPSMEFTd6.h.
|
protected |
Definition at line 6897 of file NPSMEFTd6.h.
|
protected |
Definition at line 6898 of file NPSMEFTd6.h.
|
protected |
Definition at line 6899 of file NPSMEFTd6.h.
|
protected |
Definition at line 6881 of file NPSMEFTd6.h.
|
protected |
Definition at line 6882 of file NPSMEFTd6.h.
|
protected |
Definition at line 6883 of file NPSMEFTd6.h.
|
protected |
Definition at line 6865 of file NPSMEFTd6.h.
|
protected |
Definition at line 6866 of file NPSMEFTd6.h.
|
protected |
Definition at line 6867 of file NPSMEFTd6.h.
|
protected |
Definition at line 6889 of file NPSMEFTd6.h.
|
protected |
Definition at line 6890 of file NPSMEFTd6.h.
|
protected |
Definition at line 6891 of file NPSMEFTd6.h.
|
protected |
Definition at line 6829 of file NPSMEFTd6.h.
|
protected |
Definition at line 6570 of file NPSMEFTd6.h.
|
protected |
Definition at line 6571 of file NPSMEFTd6.h.
|
protected |
Definition at line 6573 of file NPSMEFTd6.h.
|
protected |
Definition at line 6574 of file NPSMEFTd6.h.
|
protected |
Definition at line 6572 of file NPSMEFTd6.h.
|
protected |
Definition at line 6571 of file NPSMEFTd6.h.
|
protected |
Definition at line 6573 of file NPSMEFTd6.h.
|
protected |
Definition at line 6574 of file NPSMEFTd6.h.
|
protected |
Definition at line 6572 of file NPSMEFTd6.h.
|
protected |
Definition at line 6573 of file NPSMEFTd6.h.
|
protected |
Definition at line 6574 of file NPSMEFTd6.h.
|
protected |
Definition at line 6563 of file NPSMEFTd6.h.
|
protected |
Definition at line 6564 of file NPSMEFTd6.h.
|
protected |
Definition at line 6565 of file NPSMEFTd6.h.
|
protected |
Definition at line 6564 of file NPSMEFTd6.h.
|
protected |
Definition at line 6565 of file NPSMEFTd6.h.
|
protected |
Definition at line 6580 of file NPSMEFTd6.h.
|
protected |
Definition at line 6580 of file NPSMEFTd6.h.
|
protected |
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions modifying the Higgs trilinear coupling (Quadratic terms).
Definition at line 6952 of file NPSMEFTd6.h.
|
protected |
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions.
Definition at line 6950 of file NPSMEFTd6.h.
|
protected |
Definition at line 6538 of file NPSMEFTd6.h.
|
protected |
Definition at line 6539 of file NPSMEFTd6.h.
|
protected |
Definition at line 6540 of file NPSMEFTd6.h.
|
protected |
Definition at line 6539 of file NPSMEFTd6.h.
|
protected |
Definition at line 6540 of file NPSMEFTd6.h.
|
protected |
Definition at line 6539 of file NPSMEFTd6.h.
|
protected |
Definition at line 6539 of file NPSMEFTd6.h.
|
protected |
Definition at line 6540 of file NPSMEFTd6.h.
|
protected |
Definition at line 6540 of file NPSMEFTd6.h.
|
protected |
Definition at line 6308 of file NPSMEFTd6.h.
|
protected |
Definition at line 6541 of file NPSMEFTd6.h.
|
protected |
Definition at line 6542 of file NPSMEFTd6.h.
|
protected |
Definition at line 6544 of file NPSMEFTd6.h.
|
protected |
Definition at line 6545 of file NPSMEFTd6.h.
|
protected |
Definition at line 6543 of file NPSMEFTd6.h.
|
protected |
Definition at line 6542 of file NPSMEFTd6.h.
|
protected |
Definition at line 6543 of file NPSMEFTd6.h.
|
protected |
Definition at line 6542 of file NPSMEFTd6.h.
|
protected |
Definition at line 6542 of file NPSMEFTd6.h.
|
protected |
Definition at line 6544 of file NPSMEFTd6.h.
|
protected |
Definition at line 6545 of file NPSMEFTd6.h.
|
protected |
Definition at line 6543 of file NPSMEFTd6.h.
|
protected |
Definition at line 6543 of file NPSMEFTd6.h.
|
protected |
Definition at line 6544 of file NPSMEFTd6.h.
|
protected |
Definition at line 6545 of file NPSMEFTd6.h.
|
protected |
Definition at line 6546 of file NPSMEFTd6.h.
|
protected |
Definition at line 6547 of file NPSMEFTd6.h.
|
protected |
Definition at line 6549 of file NPSMEFTd6.h.
|
protected |
Definition at line 6550 of file NPSMEFTd6.h.
|
protected |
Definition at line 6548 of file NPSMEFTd6.h.
|
protected |
Definition at line 6547 of file NPSMEFTd6.h.
|
protected |
Definition at line 6548 of file NPSMEFTd6.h.
|
protected |
Definition at line 6547 of file NPSMEFTd6.h.
|
protected |
Definition at line 6547 of file NPSMEFTd6.h.
|
protected |
Definition at line 6549 of file NPSMEFTd6.h.
|
protected |
Definition at line 6550 of file NPSMEFTd6.h.
|
protected |
Definition at line 6548 of file NPSMEFTd6.h.
|
protected |
Definition at line 6548 of file NPSMEFTd6.h.
|
protected |
Definition at line 6549 of file NPSMEFTd6.h.
|
protected |
Definition at line 6550 of file NPSMEFTd6.h.
|
protected |
Definition at line 6566 of file NPSMEFTd6.h.
|
protected |
Definition at line 6567 of file NPSMEFTd6.h.
|
protected |
Definition at line 6568 of file NPSMEFTd6.h.
|
protected |
Definition at line 6567 of file NPSMEFTd6.h.
|
protected |
Definition at line 6569 of file NPSMEFTd6.h.
|
protected |
Definition at line 6568 of file NPSMEFTd6.h.
|
protected |
Definition at line 6580 of file NPSMEFTd6.h.
|
protected |
Definition at line 6580 of file NPSMEFTd6.h.
|
protected |
Definition at line 6584 of file NPSMEFTd6.h.
|
protected |
Definition at line 6584 of file NPSMEFTd6.h.
|
protected |
Definition at line 6584 of file NPSMEFTd6.h.
|
protected |
Definition at line 6584 of file NPSMEFTd6.h.
|
protected |
Definition at line 6584 of file NPSMEFTd6.h.
|
protected |
Definition at line 6584 of file NPSMEFTd6.h.
|
protected |
Definition at line 6575 of file NPSMEFTd6.h.
|
protected |
Definition at line 6576 of file NPSMEFTd6.h.
|
protected |
Definition at line 6577 of file NPSMEFTd6.h.
|
protected |
Definition at line 6576 of file NPSMEFTd6.h.
|
protected |
Definition at line 6578 of file NPSMEFTd6.h.
|
protected |
Definition at line 6578 of file NPSMEFTd6.h.
|
protected |
Definition at line 6578 of file NPSMEFTd6.h.
|
protected |
Definition at line 6579 of file NPSMEFTd6.h.
|
protected |
Definition at line 6579 of file NPSMEFTd6.h.
|
protected |
Definition at line 6579 of file NPSMEFTd6.h.
|
protected |
Definition at line 6577 of file NPSMEFTd6.h.
|
protected |
Definition at line 6581 of file NPSMEFTd6.h.
|
protected |
Definition at line 6581 of file NPSMEFTd6.h.
|
protected |
Definition at line 6581 of file NPSMEFTd6.h.
|
protected |
Definition at line 6581 of file NPSMEFTd6.h.
|
protected |
Definition at line 6581 of file NPSMEFTd6.h.
|
protected |
Definition at line 6581 of file NPSMEFTd6.h.
|
protected |
Definition at line 6581 of file NPSMEFTd6.h.
|
protected |
Definition at line 6581 of file NPSMEFTd6.h.
|
protected |
Definition at line 6581 of file NPSMEFTd6.h.
|
protected |
Definition at line 6581 of file NPSMEFTd6.h.
|
protected |
Definition at line 6583 of file NPSMEFTd6.h.
|
protected |
Definition at line 6583 of file NPSMEFTd6.h.
|
protected |
Definition at line 6583 of file NPSMEFTd6.h.
|
protected |
Definition at line 6583 of file NPSMEFTd6.h.
|
protected |
Definition at line 6583 of file NPSMEFTd6.h.
|
protected |
Definition at line 6583 of file NPSMEFTd6.h.
|
protected |
Definition at line 6583 of file NPSMEFTd6.h.
|
protected |
Definition at line 6583 of file NPSMEFTd6.h.
|
protected |
Definition at line 6583 of file NPSMEFTd6.h.
|
protected |
Definition at line 6583 of file NPSMEFTd6.h.
|
protected |
Definition at line 6585 of file NPSMEFTd6.h.
|
protected |
Definition at line 6585 of file NPSMEFTd6.h.
|
protected |
Parameter to control the inclusion of log-enhanced contributions via RG effects. If activated then it takes the value multiplying the anomalous dimension: \(-\log(\Lambda/\mu)/16 \pi^2 \Lambda^2\).
Definition at line 6954 of file NPSMEFTd6.h.
|
protected |
Another parameter to control the inclusion of log-enhanced contributions via RG effects. It multiplies the logarithmic contribution to some observables, so it takes values 0/1 to deactivate/activate the log terms.
Definition at line 6955 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{T}\).
Definition at line 6328 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{11}\) (imaginary part).
Definition at line 6472 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{11}\) (real part).
Definition at line 6466 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{12}\) (imaginary part).
Definition at line 6473 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{12}\) (real part).
Definition at line 6467 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{13}\) (imaginary part).
Definition at line 6474 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{13}\) (real part).
Definition at line 6468 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{22}\) (imaginary part).
Definition at line 6475 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{22}\) (real part).
Definition at line 6469 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{23}\) (imaginary part).
Definition at line 6476 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{23}\) (real part).
Definition at line 6470 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{33}\) (imaginary part).
Definition at line 6477 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{33}\) (real part).
Definition at line 6471 of file NPSMEFTd6.h.
|
protected |
Definition at line 6582 of file NPSMEFTd6.h.
|
protected |
Definition at line 6582 of file NPSMEFTd6.h.
|
protected |
Definition at line 6582 of file NPSMEFTd6.h.
|
protected |
Definition at line 6582 of file NPSMEFTd6.h.
|
protected |
Definition at line 6582 of file NPSMEFTd6.h.
|
protected |
Definition at line 6582 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{11}\) (imaginary part).
Definition at line 6448 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{11}\) (real part).
Definition at line 6442 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{12}\) (imaginary part).
Definition at line 6449 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{12}\) (real part).
Definition at line 6443 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{13}\) (imaginary part).
Definition at line 6450 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{13}\) (real part).
Definition at line 6444 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{22}\) (imaginary part).
Definition at line 6451 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{22}\) (real part).
Definition at line 6445 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{23}\) (imaginary part).
Definition at line 6452 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{23}\) (real part).
Definition at line 6446 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{33}\) (imaginary part).
Definition at line 6453 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{33}\) (real part).
Definition at line 6447 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{11}\) (imaginary part).
Definition at line 6424 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{11}\) (real part).
Definition at line 6418 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{12}\) (imaginary part).
Definition at line 6425 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{12}\) (real part).
Definition at line 6419 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{13}\) (imaginary part).
Definition at line 6426 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{13}\) (real part).
Definition at line 6420 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{22}\) (imaginary part).
Definition at line 6427 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{22}\) (real part).
Definition at line 6421 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{23}\) (imaginary part).
Definition at line 6428 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{23}\) (real part).
Definition at line 6422 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{33}\) (imaginary part).
Definition at line 6429 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{33}\) (real part).
Definition at line 6423 of file NPSMEFTd6.h.
|
protected |
Definition at line 6582 of file NPSMEFTd6.h.
|
protected |
Definition at line 6582 of file NPSMEFTd6.h.
|
protected |
Definition at line 6582 of file NPSMEFTd6.h.
|
protected |
Definition at line 6582 of file NPSMEFTd6.h.
|
protected |
Definition at line 6582 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{11}\) (imaginary part).
Definition at line 6460 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{11}\) (real part).
Definition at line 6454 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{12}\) (imaginary part).
Definition at line 6461 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{12}\) (real part).
Definition at line 6455 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{13}\) (imaginary part).
Definition at line 6462 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{13}\) (real part).
Definition at line 6456 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{22}\) (imaginary part).
Definition at line 6463 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{22}\) (real part).
Definition at line 6457 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{23}\) (imaginary part).
Definition at line 6464 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{23}\) (real part).
Definition at line 6458 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{33}\) (imaginary part).
Definition at line 6465 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{33}\) (real part).
Definition at line 6459 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{W}\).
Definition at line 6312 of file NPSMEFTd6.h.
|
protected |
The square of the tree level values for the cosine of the weak angle.
Definition at line 6917 of file NPSMEFTd6.h.
|
protected |
The tree level values for the cosine of the weak angle.
Definition at line 6915 of file NPSMEFTd6.h.
|
protected |
Parameters to control the SM EW input scheme: Alpha or MW.
Definition at line 6957 of file NPSMEFTd6.h.
|
protected |
Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition for EWPO.
Definition at line 6941 of file NPSMEFTd6.h.
|
protected |
Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition.
Definition at line 6937 of file NPSMEFTd6.h.
|
protected |
The \(\mathcal{O}(\Lambda^{-2})\) dimension 6 correction to the electromagnetic coupling.
\(\nc{\daEW}{\delta_{\alpha}}\) \(\nc{\dMZZ}{\delta_{M_Z^2}}\) \(\nc{\dGf}{\delta_{G_F}}\)
\[ \daEW^{(1)} = -2 s_W c_W \frac{C_{\varphi WB}\vt^2}{\Lambda^2} \]
Definition at line 7010 of file NPSMEFTd6.h.
|
protected |
The \(\mathcal{O}(\Lambda^{-4})\) dimension 6 correction to the electromagnetic coupling.
\[ \daEW^{(2)} = -2 s_W c_W \frac{C_{\varphi WB} \vt^2}{\Lambda^2} \left( \frac{\left(C_{\varphi W}+C_{\varphi B}\right)\vt^2}{\Lambda^2} + \frac{1}{4} \frac{C_{\varphi D}\vt^2}{\Lambda^2} + 3\dGf^{(1)}\right) \]
Definition at line 7020 of file NPSMEFTd6.h.
|
protected |
Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition.
Definition at line 6938 of file NPSMEFTd6.h.
|
protected |
The dimension 6 correction to the electric constant parameter.
Definition at line 6978 of file NPSMEFTd6.h.
|
protected |
The relative dimension 6 correction to the QED interaction vertex.
Definition at line 6984 of file NPSMEFTd6.h.
|
protected |
The \(\mathcal{O}(\Lambda^{-2})\) dimension 6 correction to the \(U(1)_Y\) gauge coupling, for the Alpha-Scheme (cAsch=1, cWsch=0) or the Mw-Scheme (cAsch=0, cWsch=1).
\(\nc{\daEW}{\delta_{\alpha}}\) \(\nc{\dMZZ}{\delta_{M_Z^2}}\) \(\nc{\dGf}{\delta_{G_F}}\)
\[ \gbL = \text{cAsch} \left[\gbt \frac{c_W^2\daEW^{(1)}-s_W^2\left(\dMZZ^{(1)}+\dGf^{(1)}\right)}{2(-1+2 s_W^2)} \right] + \text{cWsch} \left[\gbt \frac{-\dMZZ^{(1)}-s_W^2\dGf^{(1)}}{2 s_W^2}\right] \]
Definition at line 7057 of file NPSMEFTd6.h.
|
protected |
The \(\mathcal{O}(\Lambda^{-4})\) dimension 6 correction to the \(U(1)_Y\) gauge coupling.
Alpha-Scheme:
\begin{eqnarray*} \gbQ &=& \gbt \frac{4 (-1+2 s_W^2)^2 \left( c_W^2 \daEW^{(2)} - s_W^2\big(\dGf^{(2)} + \dMZZ^{(2)}\big) \right) + \big( -3+12s_W^2-19s_W^4+10s_W^6 \big) \left(\daEW^{(1)}\right)^2 + s_W^4\big(-7+10s_W^2\big) \left((\dMZZ^{(1)})^2+(\dGf^{(1)})^2\right)}{8(-1+2s_W^2)^3} \\ &+& \gbt \frac{ s_W^2 (3-5s_W^2+2s_W^4) \left( \daEW^{(1)}\dMZZ^{(1)} + \daEW^{(1)}\dGf^{(1)}\right) + s_W^2 (-2+s_W^2+2s_W^4) ~ \dMZZ^{(1)} ~ \dGf^{(1)}}{4(-1+2s_W^2)^3} \end{eqnarray*}
Mw-Scheme:
\[ \gbQ = \gbt \left[ -\frac{\dMZZ^{(2)}}{2s_W^2} - \frac{\dGf^{(2)}}{2} - \frac{ (1-4 s_W^2)\left(\dMZZ^{(1)}\right)^2}{8s_W^4} + \frac{3\left(\dGf^{(1)}\right)^2}{8} + \frac{\dMZZ^{(1)} \dGf^{(1)}}{4s_W^2}\right] \]
Definition at line 7076 of file NPSMEFTd6.h.
|
protected |
The \(\mathcal{O}(\Lambda^{-2})\) dimension 6 correction to the \(SU(2)_L\) gauge coupling, for the Alpha-Scheme (cAsch=1, cWsch=0) or the Mw-Scheme (cAsch=0, cWsch=1).
\[ \gwL = \text{cAsch}\left[ \gwt\left( -\frac{\daEW^{(1)}}{2} - \frac{c_W^2(-\daEW^{(1)}+\dGf^{(1)}+\dMZZ^{(1)})}{2(c_W^2-s_W^2)} \right) \right] + \text{cWsch} \left[ \gwt \left(-\frac{\dGf^{(1)}}{2}\right) \right] \]
Definition at line 7087 of file NPSMEFTd6.h.
|
protected |
The \(\mathcal{O}(\Lambda^{-4})\) dimension 6 correction to the \(SU(2)_L\) gauge coupling.
Alpha-Scheme:
\begin{eqnarray*} \gwQ &=& \gwt \frac{ 4 (-1+2s_W^2)^2 \left( -s_W^2 \daEW^{(2)} + c_W^2\big(\dGf^{(2)} + \dMZZ^{(2)}\big) \right) + s_W^2 \big(4-11s_W^2+10s_W^4\big) \left(\daEW^{(1)}\right)^2 + c_W^4 \big(-3+10s_W^2\big) \left((\dMZZ^{(1)})^2+(\dGf^{(1)})^2\right) }{8(-1+2s_W^2)^3} \\ &+& \gwt \frac{ s_W^2 \big(-1-s_W^2+2s_W^4\big) \left( \daEW^{(1)}\dMZZ^{(1)} + \daEW^{(1)}\dGf^{(1)} \right) + \big(-1+6s_W^2-7s_W^4+2s_W^6\big) ~ \dMZZ^{(1)} ~ \dGf^{(1)} }{4(-1+2s_W^2)^3} \end{eqnarray*}
Mw-Scheme:
\[ \gwQ = \gwt \left[-\frac{\dGf^{(2)}}{2} + \frac{3\left(\dGf^{(1)}\right)^2}{8}\right] \]
Definition at line 7105 of file NPSMEFTd6.h.
|
protected |
The dimension 6 correction to the Fermi constant, as extracted from muon decay.
Definition at line 6973 of file NPSMEFTd6.h.
|
protected |
The \(\mathcal{O}(\Lambda^{-4})\) dimension 6 correction to the Fermi constant.
\[ \dGf^{(2)} = \left( (C_{\varphi l}^{(3)11})^2 +(C_{\varphi l}^{(3)22})^2 +3C_{\varphi l}^{(3)11} C_{\varphi l}^{(3)22} \right) \frac{\vt^4 }{\Lambda^4} - \left(C_{\varphi l}^{(3)11} + C_{\varphi l}^{(3)22}\right) \left( C_{ll}^{1221}+C_{ll}^{2112}\right) \frac{\vt^4 }{\Lambda^4} + \frac{1}{4} \left( C_{ll}^{1221}+C_{ll}^{2112}\right)^2 \frac{\vt^4 }{\Lambda^4} \]
Definition at line 6998 of file NPSMEFTd6.h.
|
protected |
Combinations of dimension 6 coefficients modifying the \(H\) canonical field definition.
Definition at line 6944 of file NPSMEFTd6.h.
|
protected |
The dimension 6 correction to W mass Lagrangian parameter.
Definition at line 6976 of file NPSMEFTd6.h.
|
protected |
The dimension 6 correction to Z mass Lagrangian parameter.
Definition at line 6975 of file NPSMEFTd6.h.
|
protected |
The \(\mathcal{O}(\Lambda^{-2})\) dimension 6 correction to the Z-boson mass squared.
\[ \dMZZ^{(1)} = 2 s_W c_W \frac{C_{\varphi WB}\vt^2}{\Lambda^2} + \frac{1}{2} \frac{C_{\varphi D}\vt^2}{\Lambda^2} \]
Definition at line 7029 of file NPSMEFTd6.h.
|
protected |
The \(\mathcal{O}(\Lambda^{-4})\) dimension 6 correction to the Z-boson mass squared.
\begin{eqnarray*} \dMZZ^{(2)} &=& \text{cAsch} \left[ \left(3 s_W c_W C_{\varphi WB}\frac{vt^2}{\Lambda^2} + \frac{1}{2} C_{\varphi D}\frac{\vt^2}{\Lambda^2}\right)\dGf^{(1)} + 2 s_W c_W C_{\varphi WB}\left(C_{\varphi W}+C_{\varphi B}+\frac{3}{4}C_{\varphi D}\right)\frac{\vt^4}{\Lambda^4} + (1+4s_W^2 c_W^2)C_{\varphi WB}^2 \frac{\vt^4}{\Lambda^4} \right]\\ &+& \text{cWsch} \left[ \left(2s_W c_W C_{\varphi WB}\frac{\vt^2}{\Lambda^2} + \frac{1}{2} C_{\varphi D}\frac{\vt^2}{\Lambda^2} \right) \dGf^{(1)} + (1+2 c_W^2 - 4 c_W^4) C_{\varphi WB}^2 \frac{\vt^4}{\Lambda^4} + 2 s_W c_W C_{\varphi WB} \left(C_{\varphi W} + C_{\varphi B} + \frac{1}{2}C_{\varphi D}\right) \frac{\vt^4}{\Lambda^4} + \frac{(1-2 c_W^2)c_W}{2s_W} C_{\varphi WB} C_{\varphi D} \frac{\vt^4}{\Lambda^4} \right] \end{eqnarray*}
Definition at line 7043 of file NPSMEFTd6.h.
|
protected |
The dimension 6 charge correction to neutral current EW couplings.
Definition at line 6981 of file NPSMEFTd6.h.
|
protected |
The dimension 6 correction to the weak mixing angle.
Definition at line 6979 of file NPSMEFTd6.h.
|
protected |
The dimension 6 universal correction to charged current EW couplings.
Definition at line 6982 of file NPSMEFTd6.h.
|
protected |
The dimension 6 universal correction to neutral current EW couplings.
Definition at line 6980 of file NPSMEFTd6.h.
|
protected |
The dimension 6 correction to the vev, as extracted from GF.
Definition at line 6977 of file NPSMEFTd6.h.
|
protected |
The \(\mathcal{O}(\Lambda^{-2})\) dimension 6 correction to the component of the matrix that transform the gauge field \(B_{\mu}\) into \(Z_{\mu}\).
\[ \Delta \mathbb{X}_{BZ}^{(1)} = c_W^2 s_W \left(\frac{\gwL}{\gwt}-\frac{\gbL}{\gbt}\right) - c_W^3 \frac{C_{\varphi WB}\vt^2}{\Lambda^2 } \]
where, \(s_W\) and \(c_W\) are the tree level values for the sine and cosine of the weak angle. Whereas \(\gwt\) and \(\gbt\) are tree level values of the \(SU(2)_{L}\) and \(U(1)_Y\) gauge couplings at the Z-pole, and \(\Delta g^{(1)}\) their \(\mathcal{O}(\Lambda^{-2})\) new physics corrections.
Definition at line 7149 of file NPSMEFTd6.h.
|
protected |
The \(\mathcal{O}(\Lambda^{-4})\) dimension 6 correction to the component of the matrix that transform the gauge field \(B_{\mu}\) into \(Z_{\mu}\).
\begin{eqnarray*} \Delta \mathbb{X}_{BZ}^{(2)} &=& \frac{3 s_W^3 c_W^2}{2}\left(\frac{\gbL}{\gbt^2}\right)^2 + \frac{s_W c_W^2(s_W^2-2c_W^2)}{2}\left(\frac{\gwL}{\gwt}\right)^2 - s_W c_W(2s_W^2-c_W^2)\frac{\gwL}{\gwt}\frac{\gbL}{\gbt} + s_W c_W^2\left(\frac{\gwQ}{\gwt}-\frac{\gbQ}{\gbt}\right) \\ &-& 3s_W^2 c_W^3\left(\frac{\gwL}{\gwt}-\frac{\gbL}{\gbt}\right)\frac{C_{\varphi WB}\vt^2}{\Lambda^2 } - \frac{1}{2}s_W(s_W^4+3s_W^2 c_W^2- c_W^4)\frac{C_{\varphi WB}^2\vt^4}{\Lambda^4 } + c_W^3\left(C_{\varphi WB}(C_{\varphi W}+C_{\varphi B})\frac{\vt^4}{\Lambda^4} + \delta_{G_F}^{(1)} \frac{C_{\varphi WB} \vt^2}{\Lambda^2} \right) \end{eqnarray*}
where, \(s_W\) and \(c_W\) are the tree level values for the sine and cosine of the weak angle. Whereas \(\gwt\) and \(\gbt\) are tree level values of the \(SU(2)_{L}\) and \(U(1)_Y\) gauge couplings at the Z-pole; \(\Delta g^{(1)}\) and \(\Delta g^{(2)}\) their respective \(\mathcal{O}(\Lambda^{-2})\) and \(\mathcal{O}(\Lambda^{-4})\) new physics corrections.
Definition at line 7185 of file NPSMEFTd6.h.
|
protected |
The \(\mathcal{O}(\Lambda^{-2})\) dimension 6 correction to the component of the matrix that transform the gauge field \(W_{\mu}^3\) into \(Z_{\mu}\).
\[ \Delta \mathbb{X}_{WZ}^{(1)} = s_W^2 c_W \left(\frac{\gwL}{\gwt}-\frac{\gbL}{\gbt}\right) + s_W^3 \frac{C_{\varphi WB}\vt^2}{\Lambda^2 } \]
where, \(s_W\) and \(c_W\) are the tree level values for the sine and cosine of the weak angle. Whereas \(\gwt\) and \(\gbt\) are tree level values of the \(SU(2)_{L}\) and \(U(1)_Y\) gauge couplings at the Z-pole, and \(\Delta g^{(1)}\) their \(\mathcal{O}(\Lambda^{-2})\) new physics corrections.
Definition at line 7137 of file NPSMEFTd6.h.
|
protected |
The \(\mathcal{O}(\Lambda^{-4})\) dimension 6 correction to the component of the matrix that transform the gauge field \(W_{\mu}^3\) into \(Z_{\mu}\).
\begin{eqnarray*} \Delta \mathbb{X}_{WZ}^{(2)} &=& -\frac{3 s_W^2 c_W^3}{2}\left(\frac{\gwL}{\gwt}\right)^2 + \frac{s_W^2 c_W(2 s_W^2- c_W^2)}{2}\left(\frac{\gbL}{\gbt}\right)^2 - s_W^2 c_W(s_W^2-2 c_W^2)\frac{\gwL}{\gwt}\frac{\gbL}{\gbt} + s_W^2 c_W\left(\frac{\gwQ}{\gwt}-\frac{\gbQ}{\gbt}\right) \\ &-& 3 s_W^3 c_W^2 \left(\frac{\gwL}{\gwt}-\frac{\gbL}{\gbt}\right)\frac{C_{\varphi WB}\vt^2}{\Lambda^2 } -c_W(s_W^4-3s_W^2 c_W^2-c_W^4)\frac{C_{\varphi WB}\vt^4}{\Lambda^4 } + s_W^3\left(C_{\varphi WB}(C_{\varphi W}+C_{\varphi B})\frac{\vt^4}{\Lambda^4} + \delta_{G_F}^{(1)} \frac{C_{\varphi WB} \vt^2}{\Lambda^2} \right) \end{eqnarray*}
where, \(s_W\) and \(c_W\) are the tree level values for the sine and cosine of the weak angle. Whereas \(\gwt\) and \(\gbt\) are tree level values of the \(SU(2)_{L}\) and \(U(1)_Y\) gauge couplings at the Z-pole; \(\Delta g^{(1)}\) and \(\Delta g^{(2)}\) their respective \(\mathcal{O}(\Lambda^{-2})\) and \(\mathcal{O}(\Lambda^{-4})\) new physics corrections.
Definition at line 7167 of file NPSMEFTd6.h.
|
protected |
Combination of dimension 6 coefficients modifying the \(Z_\mu\) canonical field definition for EWPO.
Definition at line 6940 of file NPSMEFTd6.h.
|
protected |
Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition for EWPO.
Definition at line 6942 of file NPSMEFTd6.h.
|
protected |
Combination of dimension 6 coefficients modifying the \(Z_\mu\) canonical field definition.
Definition at line 6936 of file NPSMEFTd6.h.
|
protected |
Independent contribution to aTGC.
Definition at line 6765 of file NPSMEFTd6.h.
|
protected |
Definition at line 6971 of file NPSMEFTd6.h.
|
protected |
Definition at line 6971 of file NPSMEFTd6.h.
|
protected |
Independent contribution to aTGC.
Definition at line 6766 of file NPSMEFTd6.h.
|
protected |
Definition at line 6946 of file NPSMEFTd6.h.
|
protected |
Definition at line 6946 of file NPSMEFTd6.h.
|
protected |
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization and combinations entering in the linear and quadratic pieces.
Definition at line 6946 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(e^+ e^- \to W^+ W^-\): total cross section and \(d/d\cos{\theta}\) distribution.
Definition at line 6628 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.)
Definition at line 6602 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.)
Definition at line 6603 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.)
Definition at line 6598 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.)
Definition at line 6599 of file NPSMEFTd6.h.
|
protected |
Definition at line 6628 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.)
Definition at line 6600 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.)
Definition at line 6601 of file NPSMEFTd6.h.
|
protected |
The em coupling at Mz.
Definition at line 6913 of file NPSMEFTd6.h.
|
protected |
The em coupling squared (at Mz).
Definition at line 6914 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(e^- p \to H e^- j\) via WBF. (Assumed to be constant in energy.)
Definition at line 6604 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(e^- p \to H e^- j\) via WBF. (Assumed to be constant in energy.)
Definition at line 6605 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(e^- p \to H e^- j\) via ZBF. (Assumed to be constant in energy.)
Definition at line 6606 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(e^- p \to H e^- j\) via ZBF. (Assumed to be constant in energy.)
Definition at line 6607 of file NPSMEFTd6.h.
|
protected |
Definition at line 6630 of file NPSMEFTd6.h.
|
protected |
Definition at line 6630 of file NPSMEFTd6.h.
|
protected |
Total relative theoretical error in \(gg \to H \to X\).
Definition at line 6630 of file NPSMEFTd6.h.
|
protected |
Definition at line 6630 of file NPSMEFTd6.h.
|
protected |
Definition at line 6630 of file NPSMEFTd6.h.
|
protected |
Definition at line 6630 of file NPSMEFTd6.h.
|
protected |
Definition at line 6630 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in ggF production. (Assumed to be constant in energy.)
Definition at line 6588 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in ggF production. (Assumed to be constant in energy.)
Definition at line 6589 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to b\bar{b}\).
Definition at line 6624 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to b\bar{b}\).
Definition at line 6625 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to c\bar{c}\).
Definition at line 6622 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to c\bar{c}\).
Definition at line 6623 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to \gamma\gamma\).
Definition at line 6616 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to \gamma\gamma\).
Definition at line 6617 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to g g\).
Definition at line 6608 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to g g\).
Definition at line 6609 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to \mu^+ \mu^-\).
Definition at line 6618 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to \mu^+ \mu^-\).
Definition at line 6619 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to \tau^+ \tau^-\).
Definition at line 6620 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to \tau^+ \tau^-\).
Definition at line 6621 of file NPSMEFTd6.h.
|
protected |
Total relative theoretical error in the Higgs width.
Definition at line 6637 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to W W\).
Definition at line 6610 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to W W\).
Definition at line 6611 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to Z \gamma\).
Definition at line 6614 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to Z \gamma\).
Definition at line 6615 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to Z Z\).
Definition at line 6612 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to Z Z\).
Definition at line 6613 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (13 & 14 TeV).
Definition at line 6760 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (13 & 14 TeV).
Definition at line 6758 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (13 & 14 TeV).
Definition at line 6757 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (13 & 14 TeV).
Definition at line 6759 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (1.96 TeV).
Definition at line 6750 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (1.96 TeV).
Definition at line 6748 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (1.96 TeV).
Definition at line 6747 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (1.96 TeV).
Definition at line 6749 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (7 & 8 TeV).
Definition at line 6755 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (7 & 8 TeV).
Definition at line 6753 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (7 & 8 TeV).
Definition at line 6752 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (7 & 8 TeV).
Definition at line 6754 of file NPSMEFTd6.h.
|
protected |
Definition at line 6634 of file NPSMEFTd6.h.
|
protected |
Definition at line 6634 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in ttH production. (Assumed to be constant in energy.)
Definition at line 6590 of file NPSMEFTd6.h.
|
protected |
Total relative theoretical error in \(pp \to ttH \to tt X\).
Definition at line 6634 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in ttH production. (Assumed to be constant in energy.)
Definition at line 6591 of file NPSMEFTd6.h.
|
protected |
Definition at line 6634 of file NPSMEFTd6.h.
|
protected |
Definition at line 6634 of file NPSMEFTd6.h.
|
protected |
Definition at line 6634 of file NPSMEFTd6.h.
|
protected |
Definition at line 6634 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 6682 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 6680 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 6681 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 6676 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 6670 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 6675 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 6673 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 6679 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 6671 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 6674 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 6672 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 6677 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 6678 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 6654 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 6652 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 6653 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 6648 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 6642 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 6647 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 6645 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 6651 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 6643 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 6646 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 6644 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 6649 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 6650 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 6668 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 6666 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 6667 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 6662 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 6656 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 6661 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 6659 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 6665 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 6657 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 6660 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 6658 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 6663 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 6664 of file NPSMEFTd6.h.
|
protected |
Definition at line 6631 of file NPSMEFTd6.h.
|
protected |
Definition at line 6631 of file NPSMEFTd6.h.
|
protected |
Definition at line 6635 of file NPSMEFTd6.h.
|
protected |
Total relative theoretical error in \(pp \to Hjj (VBF) \to X jj\).
Definition at line 6631 of file NPSMEFTd6.h.
|
protected |
Definition at line 6631 of file NPSMEFTd6.h.
|
protected |
Definition at line 6631 of file NPSMEFTd6.h.
|
protected |
Definition at line 6631 of file NPSMEFTd6.h.
|
protected |
Definition at line 6631 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in VBF production. (Assumed to be constant in energy.)
Definition at line 6592 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in VBF production. (Assumed to be constant in energy.)
Definition at line 6593 of file NPSMEFTd6.h.
|
protected |
Total relative theoretical error in \(pp \to X H \to X + invisible\).
Definition at line 6635 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (13 & 14 TeV).
Definition at line 6706 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (13 & 14 TeV).
Definition at line 6705 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (13 & 14 TeV).
Definition at line 6700 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (13 & 14 TeV).
Definition at line 6702 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (13 & 14 TeV).
Definition at line 6701 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (13 & 14 TeV).
Definition at line 6703 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (13 & 14 TeV).
Definition at line 6704 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (1.96 TeV).
Definition at line 6690 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (1.96 TeV).
Definition at line 6689 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (1.96 TeV).
Definition at line 6684 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (1.96 TeV).
Definition at line 6686 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (1.96 TeV).
Definition at line 6685 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (1.96 TeV).
Definition at line 6687 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (1.96 TeV).
Definition at line 6688 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (7 & 8 TeV).
Definition at line 6698 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (7 & 8 TeV).
Definition at line 6697 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (7 & 8 TeV).
Definition at line 6692 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (7 & 8 TeV).
Definition at line 6694 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (7 & 8 TeV).
Definition at line 6693 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (7 & 8 TeV).
Definition at line 6695 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (7 & 8 TeV).
Definition at line 6696 of file NPSMEFTd6.h.
|
protected |
Definition at line 6632 of file NPSMEFTd6.h.
|
protected |
Definition at line 6632 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in WH production. (Assumed to be constant in energy.)
Definition at line 6594 of file NPSMEFTd6.h.
|
protected |
Total relative theoretical error in \(pp \to WH \to W X\).
Definition at line 6632 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in WH production. (Assumed to be constant in energy.)
Definition at line 6595 of file NPSMEFTd6.h.
|
protected |
Definition at line 6632 of file NPSMEFTd6.h.
|
protected |
Definition at line 6632 of file NPSMEFTd6.h.
|
protected |
Definition at line 6632 of file NPSMEFTd6.h.
|
protected |
Definition at line 6632 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 6745 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 6743 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 6744 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 6740 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 6734 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 6739 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 6737 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 6735 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 6738 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 6736 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 6741 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 6742 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 6719 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 6717 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 6718 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 6714 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 6708 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 6713 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 6711 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 6709 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 6712 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 6710 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 6715 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 6716 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 6732 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 6730 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 6731 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 6727 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 6721 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 6726 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 6724 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 6722 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 6725 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 6723 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 6728 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 6729 of file NPSMEFTd6.h.
|
protected |
Definition at line 6633 of file NPSMEFTd6.h.
|
protected |
Definition at line 6633 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in ZH production. (Assumed to be constant in energy.)
Definition at line 6596 of file NPSMEFTd6.h.
|
protected |
Total relative theoretical error in \(pp \to ZH \to Z X\).
Definition at line 6633 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in ZH production. (Assumed to be constant in energy.)
Definition at line 6597 of file NPSMEFTd6.h.
|
protected |
Definition at line 6633 of file NPSMEFTd6.h.
|
protected |
Definition at line 6633 of file NPSMEFTd6.h.
|
protected |
Definition at line 6633 of file NPSMEFTd6.h.
|
protected |
Definition at line 6633 of file NPSMEFTd6.h.
|
private |
A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients.
Definition at line 7251 of file NPSMEFTd6.h.
|
private |
A boolean flag that is true if including dependence on small variations of the SM parameters (dependence is linearized). Available only in selected Higgs observables.
Definition at line 7253 of file NPSMEFTd6.h.
|
private |
An internal boolean flag that is true if assuming lepton flavour universality.
Definition at line 7263 of file NPSMEFTd6.h.
|
private |
A boolean flag that is true if including quadratic modifications in the SM loops in Higgs observables due to the dim 6 interactions that contribute to the trilinear Higgs coupling.
Definition at line 7255 of file NPSMEFTd6.h.
|
private |
A boolean flag that is true if including modifications in the SM loops in Higgs observables due to the dim 6 interactions.
Definition at line 7254 of file NPSMEFTd6.h.
|
private |
A boolean for the model flag MWinput.
Definition at line 7257 of file NPSMEFTd6.h.
|
private |
A boolean flag that is true if assuming partial quark flavour universality between the 1st and 2nd family in the CHF operators.
Definition at line 7250 of file NPSMEFTd6.h.
|
private |
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on.
Definition at line 7248 of file NPSMEFTd6.h.
|
private |
An internal boolean flag that is true if assuming quark flavour universality.
Definition at line 7269 of file NPSMEFTd6.h.
|
private |
A flag that is TRUE if including log-enhanced 1-loop corrections propotional to the dim-6 Wilson coefficients. See comment in documentation above.
Definition at line 7256 of file NPSMEFTd6.h.
|
private |
A boolean flag that is true if we use as parameters CHWHB_gaga and CHWHB_gagaorth instead of CHW and CHB.
Definition at line 7249 of file NPSMEFTd6.h.
|
private |
A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients and all proportional to the same coefficient (CuH_33 and CuV_33 respectively).
Definition at line 7252 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(U(1)_Y\) gauge coupling contant (at the \(Z\) pole).
Definition at line 6920 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(SU(2)_L\) gauge coupling contant (at the \(Z\) pole).
Definition at line 6921 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(SU(3)_c\) gauge coupling contant (at the \(Z\) pole).
Definition at line 6922 of file NPSMEFTd6.h.
|
protected |
Definition at line 6877 of file NPSMEFTd6.h.
|
protected |
Definition at line 6878 of file NPSMEFTd6.h.
|
protected |
Definition at line 6879 of file NPSMEFTd6.h.
|
protected |
Definition at line 6846 of file NPSMEFTd6.h.
|
protected |
Definition at line 6847 of file NPSMEFTd6.h.
|
protected |
Definition at line 6861 of file NPSMEFTd6.h.
|
protected |
Definition at line 6862 of file NPSMEFTd6.h.
|
protected |
Definition at line 6863 of file NPSMEFTd6.h.
|
protected |
Definition at line 6833 of file NPSMEFTd6.h.
|
protected |
Definition at line 6855 of file NPSMEFTd6.h.
|
protected |
Definition at line 6844 of file NPSMEFTd6.h.
|
protected |
Definition at line 6853 of file NPSMEFTd6.h.
|
protected |
Definition at line 6854 of file NPSMEFTd6.h.
|
protected |
Definition at line 6825 of file NPSMEFTd6.h.
|
protected |
Definition at line 6826 of file NPSMEFTd6.h.
|
protected |
Definition at line 6827 of file NPSMEFTd6.h.
|
protected |
Definition at line 6809 of file NPSMEFTd6.h.
|
protected |
Definition at line 6810 of file NPSMEFTd6.h.
|
protected |
Definition at line 6811 of file NPSMEFTd6.h.
|
protected |
Definition at line 6842 of file NPSMEFTd6.h.
|
protected |
Definition at line 6784 of file NPSMEFTd6.h.
|
protected |
Definition at line 6785 of file NPSMEFTd6.h.
|
protected |
Definition at line 6786 of file NPSMEFTd6.h.
|
protected |
Definition at line 6787 of file NPSMEFTd6.h.
|
protected |
Definition at line 6788 of file NPSMEFTd6.h.
|
protected |
Definition at line 6789 of file NPSMEFTd6.h.
|
protected |
Definition at line 6798 of file NPSMEFTd6.h.
|
protected |
Definition at line 6799 of file NPSMEFTd6.h.
|
protected |
Definition at line 6800 of file NPSMEFTd6.h.
|
protected |
Definition at line 6801 of file NPSMEFTd6.h.
|
protected |
Definition at line 6802 of file NPSMEFTd6.h.
|
protected |
Definition at line 6803 of file NPSMEFTd6.h.
|
protected |
Definition at line 6817 of file NPSMEFTd6.h.
|
protected |
Definition at line 6818 of file NPSMEFTd6.h.
|
protected |
Definition at line 6819 of file NPSMEFTd6.h.
|
protected |
Definition at line 6843 of file NPSMEFTd6.h.
|
protected |
Definition at line 6845 of file NPSMEFTd6.h.
|
protected |
Definition at line 6908 of file NPSMEFTd6.h.
|
protected |
Definition at line 6901 of file NPSMEFTd6.h.
|
protected |
Definition at line 6902 of file NPSMEFTd6.h.
|
protected |
Definition at line 6903 of file NPSMEFTd6.h.
|
protected |
Definition at line 6885 of file NPSMEFTd6.h.
|
protected |
Definition at line 6886 of file NPSMEFTd6.h.
|
protected |
Definition at line 6887 of file NPSMEFTd6.h.
|
protected |
Definition at line 6869 of file NPSMEFTd6.h.
|
protected |
Definition at line 6870 of file NPSMEFTd6.h.
|
protected |
Definition at line 6871 of file NPSMEFTd6.h.
|
protected |
Definition at line 6893 of file NPSMEFTd6.h.
|
protected |
Definition at line 6894 of file NPSMEFTd6.h.
|
protected |
Definition at line 6895 of file NPSMEFTd6.h.
|
protected |
Definition at line 6832 of file NPSMEFTd6.h.
|
protected |
NP contributions and Total to Higgs width ratio with SM.
Definition at line 6971 of file NPSMEFTd6.h.
|
protected |
Definition at line 6931 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(Z\bar{d}d\) couplings in the SM.
Definition at line 6931 of file NPSMEFTd6.h.
|
protected |
Definition at line 6929 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(Z\ell^+\ell^-\) couplings in the SM.
Definition at line 6929 of file NPSMEFTd6.h.
|
protected |
Definition at line 6930 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(Z\bar{u}u\) couplings in the SM.
Definition at line 6930 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(Z\bar{\nu}\nu\) couplings in the SM.
Definition at line 6928 of file NPSMEFTd6.h.
|
protected |
The new physics scale [GeV].
Definition at line 6586 of file NPSMEFTd6.h.
|
protected |
The SM tree level value of the scalar quartic coupling in the potential.
Definition at line 6926 of file NPSMEFTd6.h.
|
protected |
The square of the new physics scale [GeV \(^2\)].
Definition at line 6773 of file NPSMEFTd6.h.
|
protected |
Independent contribution to aTGC.
Definition at line 6767 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(W\) boson mass.
Definition at line 6924 of file NPSMEFTd6.h.
|
static |
|
static |
The number of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities.
Definition at line 1076 of file NPSMEFTd6.h.
|
mutableprotected |
Definition at line 6298 of file NPSMEFTd6.h.
|
static |
A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotateCHWCHB=false.
Definition at line 1064 of file NPSMEFTd6.h.
|
static |
A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=false.
Definition at line 1083 of file NPSMEFTd6.h.
|
static |
A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotateCHWCHB=true.
Definition at line 1070 of file NPSMEFTd6.h.
|
static |
A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=true.
Definition at line 1090 of file NPSMEFTd6.h.
|
protected |
Definition at line 6639 of file NPSMEFTd6.h.
|
protected |
Nuisance parameters to be used in observables.
Definition at line 6639 of file NPSMEFTd6.h.
|
protected |
Definition at line 6639 of file NPSMEFTd6.h.
|
protected |
Definition at line 6639 of file NPSMEFTd6.h.
|
protected |
Definition at line 6639 of file NPSMEFTd6.h.
|
protected |
Definition at line 6639 of file NPSMEFTd6.h.
|
protected |
Definition at line 6639 of file NPSMEFTd6.h.
|
protected |
Definition at line 6639 of file NPSMEFTd6.h.
|
protected |
Definition at line 6639 of file NPSMEFTd6.h.
|
protected |
Definition at line 6639 of file NPSMEFTd6.h.
|
protected |
The square of the tree level values for the sine of the weak angle.
Definition at line 6918 of file NPSMEFTd6.h.
|
protected |
The tree level values for the sine of the weak angle.
Definition at line 6916 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(W^-\bar{\ell}\nu\) couplings in the SM. (Neglecting PMNS effects.)
Definition at line 6933 of file NPSMEFTd6.h.
|
protected |
The square of the EW vev.
Definition at line 6910 of file NPSMEFTd6.h.
|
protected |
The ratio between the EW vev and the new physics scale, squared \(v^2/\Lambda^2\).
Definition at line 6911 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(W^+\bar{u}d\) couplings in the SM. (Neglecting CKM effects.)
Definition at line 6934 of file NPSMEFTd6.h.
|
private |
Gsl integral variable
Definition at line 7271 of file NPSMEFTd6.h.
|
protected |
The tree level component of the matrix that transform the gauge field \(B_{\mu}\) into \(Z_{\mu}\).
\[ \mathbb{\widetilde{X}}_{(BZ)} = - s_W \]
where, \(s_W\) is the tree level value for the sine of the weak angle.
Definition at line 7125 of file NPSMEFTd6.h.
|
protected |
The tree level component of the matrix that transform the gauge field \(W_{\mu}^3\) into \(Z_{\mu}\).
\[ \mathbb{\widetilde{X}}_{(WZ)} = c_W \]
where, \(c_W\) is the tree level value for the cosine of the weak angle.
Definition at line 7115 of file NPSMEFTd6.h.
|
protected |
SM d-quark Yukawas.
Definition at line 6961 of file NPSMEFTd6.h.
|
protected |
Definition at line 6960 of file NPSMEFTd6.h.
|
protected |
Definition at line 6961 of file NPSMEFTd6.h.
|
protected |
Definition at line 6959 of file NPSMEFTd6.h.
|
protected |
Definition at line 6959 of file NPSMEFTd6.h.
|
protected |
Definition at line 6961 of file NPSMEFTd6.h.
|
protected |
SM u-quark Yukawas.
Definition at line 6960 of file NPSMEFTd6.h.
|
protected |
SM lepton Yukawas.
Definition at line 6959 of file NPSMEFTd6.h.
|
protected |
Definition at line 6960 of file NPSMEFTd6.h.
1.9.2 